---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '22262'
abstract:
- lang: eng
  text: Mixed modes are observed in many low-mass evolved stars. They provide information
    about core rotation rates of these stars, which are lower than predicted by stellar
    evolution models. The mixed modes themselves have been invoked as an angular momentum
    (AM) transport mechanism, but estimating their transport efficiency requires knowledge
    of their amplitudes. We constrain, for the first time, the mixed-mode amplitudes
    in 2D hydrodynamical simulations of a 1.3M⊙ red giant using the code MUSIC. We
    perform two simulations with outer radial truncations at fractional radii ro/r⋆
    = 0.90 and 0.98. We compare the modes in the simulation with those found using
    both GYRE and a Dedalus eigenvalue solver. Excellent frequency agreement is found
    for all p-dominated modes, with minor discrepancies for g-dominated modes, especially
    in the frequency range [60, 240] μHz. We find excellent eigenfunction agreement
    for all modes except those in this frequency range. According to empirical predictions,
    the largest kinetic energies are located around Vmax= 312.μHz, but in both simulations,
    the modes with frequencies of ν < 50 μHz have the largest kinetic energies. In
    the simulation with r/r⋆ = 0.98, the simulated modes have extrapolated surface
    velocities comparable to the empirical predictions, with the highest surface velocities
    in a bell-shaped curve peaking around ν = 700 μHz. The extrapolated surface velocities
    of the low-frequency modes are small and thus hard to observe, but their large
    kinetic energies deeper in the interior could significantly impact AM transport,
    which has not yet been investigated.
acknowledgement: 'We would like to thank the referee for their careful reading of
  the manuscript and their constructive comments that helped improve the paper. N.B.V.
  would like to thank K. Belkacem and J. Philidet for helpful discussions. N.B.V.
  is supported by STFC grant ST/Y002164/1. A.L.S. acknowledges support from the European
  Research Council (ERC) under the Horizon Europe program (Synergy grant agreement
  101071505: 4D-STAR) from the CNES SOHO-GOLF and PLATO grants at CEA-DAp, and from
  ATPS (CNRS/INSU). Part of this work was supported by the ERC grant No. 787361-COBOM.
  R.H.D.T. acknowledges support from NASA grants 80NSSC24K0895 and 80NSSC23K1517,
  and NSF grant 2407636. A.L. is supported by ERC Starting Grant 101165631 (“Calcifer”).
  The authors would like to acknowledge the use of the University of Exeter High-Performance
  Computing (HPC) facility, ISCA, in carrying out this work. This work used the DiRAC
  Memory Intensive service (Cosma8) at Durham University, managed by the Institute
  for Computational Cosmology, and the DiRAC Data Intensive service (DIaL3) at the
  University of Leicester, managed by the University of Leicester Research Computing
  Service. These facilities are managed on behalf of the STFC DiRAC HPC (www.dirac.ac.uk).
  The DiRAC services at Durham and Leicester were funded by BEIS, UKRI, and STFC capital
  funding, and STFC operations grants. The service at Durham received funding from
  Durham University. DiRAC is part of the UKRI Digital Research Infrastructure.'
article_number: '154'
article_processing_charge: Yes
article_type: original
arxiv: 1
author:
- first_name: Nils B.
  full_name: De Vries, Nils B.
  last_name: De Vries
- first_name: Arthur
  full_name: Le Saux, Arthur
  last_name: Le Saux
- first_name: Isabelle
  full_name: Baraffe, Isabelle
  last_name: Baraffe
- first_name: Thomas
  full_name: Guillet, Thomas
  last_name: Guillet
- first_name: Richard H.D.
  full_name: Townsend, Richard H.D.
  last_name: Townsend
- first_name: Armand
  full_name: Leclerc, Armand
  id: 2a1fb1fc-f373-11ef-901a-87cee43a1217
  last_name: Leclerc
- first_name: Adrien
  full_name: Morison, Adrien
  last_name: Morison
citation:
  ama: De Vries NB, Le Saux A, Baraffe I, et al. Revealing mixed modes in compressible
    hydrodynamical simulations of red giant stars. <i>The Astrophysical Journal</i>.
    2026;1005(2). doi:<a href="https://doi.org/10.3847/1538-4357/ae7a3c">10.3847/1538-4357/ae7a3c</a>
  apa: De Vries, N. B., Le Saux, A., Baraffe, I., Guillet, T., Townsend, R. H. D.,
    Leclerc, A., &#38; Morison, A. (2026). Revealing mixed modes in compressible hydrodynamical
    simulations of red giant stars. <i>The Astrophysical Journal</i>. IOP Publishing.
    <a href="https://doi.org/10.3847/1538-4357/ae7a3c">https://doi.org/10.3847/1538-4357/ae7a3c</a>
  chicago: De Vries, Nils B., Arthur Le Saux, Isabelle Baraffe, Thomas Guillet, Richard
    H.D. Townsend, Armand Leclerc, and Adrien Morison. “Revealing Mixed Modes in Compressible
    Hydrodynamical Simulations of Red Giant Stars.” <i>The Astrophysical Journal</i>.
    IOP Publishing, 2026. <a href="https://doi.org/10.3847/1538-4357/ae7a3c">https://doi.org/10.3847/1538-4357/ae7a3c</a>.
  ieee: N. B. De Vries <i>et al.</i>, “Revealing mixed modes in compressible hydrodynamical
    simulations of red giant stars,” <i>The Astrophysical Journal</i>, vol. 1005,
    no. 2. IOP Publishing, 2026.
  ista: De Vries NB, Le Saux A, Baraffe I, Guillet T, Townsend RHD, Leclerc A, Morison
    A. 2026. Revealing mixed modes in compressible hydrodynamical simulations of red
    giant stars. The Astrophysical Journal. 1005(2), 154.
  mla: De Vries, Nils B., et al. “Revealing Mixed Modes in Compressible Hydrodynamical
    Simulations of Red Giant Stars.” <i>The Astrophysical Journal</i>, vol. 1005,
    no. 2, 154, IOP Publishing, 2026, doi:<a href="https://doi.org/10.3847/1538-4357/ae7a3c">10.3847/1538-4357/ae7a3c</a>.
  short: N.B. De Vries, A. Le Saux, I. Baraffe, T. Guillet, R.H.D. Townsend, A. Leclerc,
    A. Morison, The Astrophysical Journal 1005 (2026).
das_tickbox: '1'
dataavailabilitystatement: The kinetic energies and surface velocities shown in Figure
  4, as well as the underlying spectral data of this work, can be found in a Zenodo
  repository at doi:10.5281/zenodo.18661976.
date_created: 2026-07-12T22:02:17Z
date_published: 2026-07-10T00:00:00Z
date_updated: 2026-07-13T08:16:25Z
day: '10'
ddc:
- '520'
department:
- _id: LiBu
doi: 10.3847/1538-4357/ae7a3c
external_id:
  arxiv:
  - '2606.07125'
file:
- access_level: open_access
  checksum: d32061d2341bac3adeb404975c6bd59e
  content_type: application/pdf
  creator: dernst
  date_created: 2026-07-13T08:14:01Z
  date_updated: 2026-07-13T08:14:01Z
  file_id: '22275'
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  success: 1
file_date_updated: 2026-07-13T08:14:01Z
has_accepted_license: '1'
intvolume: '      1005'
issue: '2'
keyword:
- Stellar physics
- Stellar interiors
- Asteroseismology
- Stellar oscillations
- Hydrodynamical simulations
language:
- iso: eng
month: '07'
oa: 1
oa_version: Published Version
project:
- _id: 914d8549-16d5-11f0-9cad-bbe6324c93a9
  grant_number: '101165631'
  name: 'Unveiling the mysteries of stellar dynamics: a pioneering journey in magnetoasteroseismology'
publication: The Astrophysical Journal
publication_identifier:
  eissn:
  - 1538-4357
  issn:
  - 0004-637X
publication_status: published
publisher: IOP Publishing
quality_controlled: '1'
researchdata_availability: yes
scopus_import: '1'
status: public
supplementarymaterial: yes
title: Revealing mixed modes in compressible hydrodynamical simulations of red giant
  stars
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 1005
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
_id: '22261'
abstract:
- lang: eng
  text: 'Climate change is significantly altering regional precipitation patterns
    across Europe and the Mediterranean. We analyze daily precipitation distribution
    changes in a 15-member Euro-CORDEX ensemble, through a diagnostic framework that
    separates occurrence changes, wet-days intensity shifts and distortions. At +4
    ∘C global warming, Northern Europe shows a robust intensification of precipitation,
    driven by both higher occurrence and stronger events. Conversely, the Mediterranean
    exhibits a dominant drying signal, primarily due to fewer wet-days, which impacts
    daily precipitation distribution even for heavy rainfall. Transitional zones in
    the northern Mediterranean reveal “U-shape” regimes, with rising extremes but
    declining moderate rain. Comparing with ERA5 reanalysis over the past, low model
    agreement in the south highlights higher uncertainty in the Mediterranean region.
    The timing of robust signal emergence varies: Northern Europe shows robust patterns
    from +1 ∘C, while the Mediterranean exhibits delays until +3-4 ∘C. These findings
    are essential for informing risk-based adaptation strategies.'
acknowledgement: J.A. gratefully acknowledges the JSPS postdoctoral fellowship (Japan
  Society for Promotion of Science, grant number P25709). C.J.M. gratefully acknowledges
  funding from the European Research Council (ERC) under the European Union’s Horizon
  2020 research and innovation program (Project CLUSTER, Grant Agreement No. 805041).
  The authors also thank Samuel Somot (Centre National de Recherches Météorologiques,
  Toulouse) and Juliette Blanchet (Institut des Géosciences de l’Environnement, Grenoble)
  for their fruitful discussions on the project.
article_number: '572'
article_processing_charge: Yes
article_type: original
author:
- first_name: Julie
  full_name: André, Julie
  last_name: André
- first_name: Nicolas
  full_name: Chiabrando, Nicolas
  last_name: Chiabrando
- first_name: Caroline J
  full_name: Muller, Caroline J
  id: f978ccb0-3f7f-11eb-b193-b0e2bd13182b
  last_name: Muller
  orcid: 0000-0001-5836-5350
- first_name: Philippe
  full_name: Drobinski, Philippe
  last_name: Drobinski
- first_name: Fabio
  full_name: D’Andrea, Fabio
  last_name: D’Andrea
citation:
  ama: André J, Chiabrando N, Muller CJ, Drobinski P, D’Andrea F. Distinct regimes
    of precipitation changes across Europe and the Mediterranean under global warming.
    <i>Communications Earth and Environment</i>. 2026;7. doi:<a href="https://doi.org/10.1038/s43247-026-03519-7">10.1038/s43247-026-03519-7</a>
  apa: André, J., Chiabrando, N., Muller, C. J., Drobinski, P., &#38; D’Andrea, F.
    (2026). Distinct regimes of precipitation changes across Europe and the Mediterranean
    under global warming. <i>Communications Earth and Environment</i>. Springer Nature.
    <a href="https://doi.org/10.1038/s43247-026-03519-7">https://doi.org/10.1038/s43247-026-03519-7</a>
  chicago: André, Julie, Nicolas Chiabrando, Caroline J Muller, Philippe Drobinski,
    and Fabio D’Andrea. “Distinct Regimes of Precipitation Changes across Europe and
    the Mediterranean under Global Warming.” <i>Communications Earth and Environment</i>.
    Springer Nature, 2026. <a href="https://doi.org/10.1038/s43247-026-03519-7">https://doi.org/10.1038/s43247-026-03519-7</a>.
  ieee: J. André, N. Chiabrando, C. J. Muller, P. Drobinski, and F. D’Andrea, “Distinct
    regimes of precipitation changes across Europe and the Mediterranean under global
    warming,” <i>Communications Earth and Environment</i>, vol. 7. Springer Nature,
    2026.
  ista: André J, Chiabrando N, Muller CJ, Drobinski P, D’Andrea F. 2026. Distinct
    regimes of precipitation changes across Europe and the Mediterranean under global
    warming. Communications Earth and Environment. 7, 572.
  mla: André, Julie, et al. “Distinct Regimes of Precipitation Changes across Europe
    and the Mediterranean under Global Warming.” <i>Communications Earth and Environment</i>,
    vol. 7, 572, Springer Nature, 2026, doi:<a href="https://doi.org/10.1038/s43247-026-03519-7">10.1038/s43247-026-03519-7</a>.
  short: J. André, N. Chiabrando, C.J. Muller, P. Drobinski, F. D’Andrea, Communications
    Earth and Environment 7 (2026).
das_tickbox: '1'
dataavailabilitystatement: ERA5 reanalysis and Euro-CORDEX simulations are publicly
  available from https://doi.org/10.24381/cds.143582cf and https://cordex.org/data-access/esgf/.
  The custom code developed and used for this paper can be accessed through Zenodo,
  https://doi.org/10.5281/zenodo.18995401.
date_created: 2026-07-12T22:02:16Z
date_published: 2026-07-06T00:00:00Z
date_updated: 2026-07-13T07:13:21Z
day: '06'
ddc:
- '550'
department:
- _id: CaMu
doi: 10.1038/s43247-026-03519-7
ec_funded: 1
file:
- access_level: open_access
  checksum: fd8f57cbe180f7a4d49ab17b3571ad2b
  content_type: application/pdf
  creator: dernst
  date_created: 2026-07-13T07:12:35Z
  date_updated: 2026-07-13T07:12:35Z
  file_id: '22272'
  file_name: 2026_CommEarthEnvironment_Andre.pdf
  file_size: 3870924
  relation: main_file
  success: 1
file_date_updated: 2026-07-13T07:12:35Z
has_accepted_license: '1'
intvolume: '         7'
language:
- iso: eng
month: '07'
oa: 1
oa_version: Published Version
project:
- _id: 629205d8-2b32-11ec-9570-e1356ff73576
  call_identifier: H2020
  grant_number: '805041'
  name: Organization of CLoUdS, and implications of Tropical  cyclones and for the
    Energetics of the tropics, in current and waRming climate
publication: Communications Earth and Environment
publication_identifier:
  eissn:
  - 2662-4435
publication_status: published
publisher: Springer Nature
quality_controlled: '1'
researchdata_availability: yes
scopus_import: '1'
status: public
supplementarymaterial: yes
title: Distinct regimes of precipitation changes across Europe and the Mediterranean
  under global warming
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 7
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '22270'
abstract:
- lang: eng
  text: "The explosion of a white dwarf (WD) in a close binary can launch a surviving
    runaway star at\r\nvelocities of ≳ 1000 km s−1\r\n. Such runaways provide a direct
    probe of thermonuclear supernovae (SNe)\r\nin double-degenerate binaries. Several
    candidate runaways are known, but their evolutionary states\r\nand the demographics
    of the broader population are uncertain. To enable robust population inference,\r\nwe
    carry out a systematic survey for hypervelocity runaways with a simple selection
    function, selecting\r\ncandidates based on large Gaia-inferred tangential velocities
    and blue colors. We classify 100% of the\r\nresulting 92 candidates using a combination
    of spectroscopic follow-up and archival data. The search\r\nyields ten suspected
    D6\r\nstars and three LP 40-365 stars. Three D6\r\nstars are new discoveries,
    including\r\ntwo hot (Teff ≳ 50,000 K) objects and one cool (Teff ≈ 7,000 K) object.
    We forward-model our survey\r\nunder several proposed D6\r\nstar evolutionary
    models, coupling each to a Galactic model and the survey\r\nselection function.
    No single model reproduces the observed diversity of D6\r\nstars, which likely
    reflects\r\na range of remnant masses, ages, and heating mechanisms. Models in
    which runaway companions\r\nare heated by SN shocks alone are too faint and short-lived
    to explain most of the observed sample,\r\nwhile fully reheated models are too
    luminous and long-lived. Models with intermediate heating,\r\nas occurs in some
    simulations of violent mergers and partially disrupted remnants, best match the\r\nobserved
    magnitude, distance, and kinematic-age distributions. The inferred D6\r\nstar
    birth rate is\r\nmodel dependent, but the models that best match the observed
    population require rates of only a\r\nfew percent of the Galactic SN Ia rate,
    perhaps implying that most SNe Ia result from WD binaries\r\nin which both components
    explode. If most SNe Ia do produce surviving runaways, these must be\r\nfainter
    or shorter-lived than the currently known runaways."
acknowledgement: "We thank Lars Bildsten, Evan Bauer, Ruediger Pakmor, Jim Fuller,
  Logan Proust, Abinaya Rajamuthukumar, and Stephan Geier for useful discussion related
  to\r\nthis work.\r\nThis work was supported by NSF grants AST-2508988\r\nand AST-2205631,
  NASA/ESA Hubble Space Telescope\r\nprogram No. 17441, and Scialog grant #SA-LSST-2024-\r\n114c
  from the Research Corporation for Science Advancement. The Kavli Institute for Theoretical
  Physics\r\n(KITP) hosted the program, “White Dwarfs as Probes of\r\nthe Evolution
  of Planets, Stars, the Milky Way, and the\r\nExpanding Universe,” during which this
  project was initiated. This research was supported in part by the U.S.\r\nNational
  Science Foundation (NSF) under grants PHY1748958. This research benefited from discussions
  that\r\nwere funded by the Gordon and Betty Moore Foundation\r\nthrough Grant GBMF5076.\r\nWe
  thank the staffs of the various observatories at\r\nwhich data were obtained. This
  work is partially based\r\non observations obtained at the Southern Astrophysical
  Research (SOAR) telescope, which is a joint project\r\nof the Minist´erio da Ciˆencia,
  Tecnologia e Inova¸c˜oes\r\n(MCTI/LNA) do Brasil, the US National Science Foundation’s
  NOIRLab, the University of North Carolina\r\nat Chapel Hill (UNC), and Michigan
  State University\r\n(MSU). Some of the data presented herein were obtained\r\nat
  the W. M. Keck Observatory, which is operated as a\r\nscientific partnership among
  the California Institute of\r\nTechnology, the University of California, and NASA;
  the observatory was made possible by the generous financial\r\nsupport of the W.
  M. Keck Foundation.\r\nThis research has made use of the Keck Observatory\r\nArchive
  (KOA), which is operated by the W. M. Keck\r\nObservatory and the NASA Exoplanet
  Science Institute\r\n(NExScI), under contract with the National Aeronautics\r\nand
  Space Administration.\r\nThis work has made use of data from the\r\nEuropean Space
  Agency (ESA) mission Gaia\r\n(https://www.cosmos.esa.int/gaia), processed\r\nby
  the Gaia Data Processing and Analysis Consortium\r\n(DPAC, https://www.cosmos.esa.int/web/gaia/\r\ndpac/consortium).
  Funding for the DPAC has been\r\nprovided by national institutions, in particular
  the\r\ninstitutions participating in the Gaia Multilateral\r\nAgreement."
article_processing_charge: No
article_type: original
arxiv: 1
author:
- first_name: Kareem
  full_name: El-Badry, Kareem
  last_name: El-Badry
- first_name: Klaus
  full_name: Werner, Klaus
  last_name: Werner
- first_name: Ken J.
  full_name: Shen, Ken J.
  last_name: Shen
- first_name: Jay
  full_name: Strader, Jay
  last_name: Strader
- first_name: Antonio C.
  full_name: Rodriguez, Antonio C.
  last_name: Rodriguez
- first_name: Jiwon Jesse
  full_name: Han, Jiwon Jesse
  last_name: Han
- first_name: Vedant
  full_name: Chandra, Vedant
  last_name: Chandra
- first_name: Laura
  full_name: Chomiuk, Laura
  last_name: Chomiuk
- first_name: Zachary P.
  full_name: Vanderbosch, Zachary P.
  last_name: Vanderbosch
- first_name: Lisa
  full_name: Blomberg, Lisa
  last_name: Blomberg
- first_name: Natsuko
  full_name: Yamaguchi, Natsuko
  last_name: Yamaguchi
- first_name: Pranav
  full_name: Nagarajan, Pranav
  last_name: Nagarajan
- first_name: Ilaria
  full_name: Caiazzo, Ilaria
  id: 8ae5b6e7-2a03-11ee-914d-b58ed7a3b47d
  last_name: Caiazzo
  orcid: 0000-0002-4770-5388
- first_name: Joannes C
  full_name: van Roestel, Joannes C
  id: 4d122fc8-6083-11f0-87a5-97d68b860333
  last_name: van Roestel
- first_name: Hila
  full_name: Glanz, Hila
  last_name: Glanz
- first_name: Tin Long Sunny
  full_name: Wong, Tin Long Sunny
  last_name: Wong
- first_name: Aakash
  full_name: Bhat, Aakash
  last_name: Bhat
- first_name: Mark A.
  full_name: Hollands, Mark A.
  last_name: Hollands
citation:
  ama: El-Badry K, Werner K, Shen KJ, et al. A systematic survey for hypervelocity
    runaways from thermonuclear supernovae. <i>The Open Journal of Astrophysics</i>.
    2026;9. doi:<a href="https://doi.org/10.33232/001c.164326">10.33232/001c.164326</a>
  apa: El-Badry, K., Werner, K., Shen, K. J., Strader, J., Rodriguez, A. C., Han,
    J. J., … Hollands, M. A. (2026). A systematic survey for hypervelocity runaways
    from thermonuclear supernovae. <i>The Open Journal of Astrophysics</i>. Maynooth
    Academic Publishing. <a href="https://doi.org/10.33232/001c.164326">https://doi.org/10.33232/001c.164326</a>
  chicago: El-Badry, Kareem, Klaus Werner, Ken J. Shen, Jay Strader, Antonio C. Rodriguez,
    Jiwon Jesse Han, Vedant Chandra, et al. “A Systematic Survey for Hypervelocity
    Runaways from Thermonuclear Supernovae.” <i>The Open Journal of Astrophysics</i>.
    Maynooth Academic Publishing, 2026. <a href="https://doi.org/10.33232/001c.164326">https://doi.org/10.33232/001c.164326</a>.
  ieee: K. El-Badry <i>et al.</i>, “A systematic survey for hypervelocity runaways
    from thermonuclear supernovae,” <i>The Open Journal of Astrophysics</i>, vol.
    9. Maynooth Academic Publishing, 2026.
  ista: El-Badry K, Werner K, Shen KJ, Strader J, Rodriguez AC, Han JJ, Chandra V,
    Chomiuk L, Vanderbosch ZP, Blomberg L, Yamaguchi N, Nagarajan P, Caiazzo I, van
    Roestel JC, Glanz H, Wong TLS, Bhat A, Hollands MA. 2026. A systematic survey
    for hypervelocity runaways from thermonuclear supernovae. The Open Journal of
    Astrophysics. 9.
  mla: El-Badry, Kareem, et al. “A Systematic Survey for Hypervelocity Runaways from
    Thermonuclear Supernovae.” <i>The Open Journal of Astrophysics</i>, vol. 9, Maynooth
    Academic Publishing, 2026, doi:<a href="https://doi.org/10.33232/001c.164326">10.33232/001c.164326</a>.
  short: K. El-Badry, K. Werner, K.J. Shen, J. Strader, A.C. Rodriguez, J.J. Han,
    V. Chandra, L. Chomiuk, Z.P. Vanderbosch, L. Blomberg, N. Yamaguchi, P. Nagarajan,
    I. Caiazzo, J.C. van Roestel, H. Glanz, T.L.S. Wong, A. Bhat, M.A. Hollands, The
    Open Journal of Astrophysics 9 (2026).
das_tickbox: '1'
dataavailabilitystatement: "We thank the staffs of the various observatories at\r\nwhich
  data were obtained. This work is partially based\r\non observations obtained at
  the Southern Astrophysical Research (SOAR) telescope, which is a joint project\r\nof
  the Minist´erio da Ciˆencia, Tecnologia e Inova¸c˜oes\r\n(MCTI/LNA) do Brasil, the
  US National Science Foundation’s NOIRLab, the University of North Carolina\r\nat
  Chapel Hill (UNC), and Michigan State University\r\n(MSU). Some of the data presented
  herein were obtained\r\nat the W. M. Keck Observatory, which is operated as a\r\nscientific
  partnership among the California Institute of\r\nTechnology, the University of California,
  and NASA; the\r\nobservatory was made possible by the generous financial\r\nsupport
  of the W. M. Keck Foundation.\r\nThis research has made use of the Keck Observatory\r\nArchive
  (KOA), which is operated by the W. M. Keck\r\nObservatory and the NASA Exoplanet
  Science Institute\r\n(NExScI), under contract with the National Aeronautics\r\nand
  Space Administration.\r\nThis work has made use of data from the\r\nEuropean Space
  Agency (ESA) mission Gaia\r\n(https://www.cosmos.esa.int/gaia), processed\r\nby
  the Gaia Data Processing and Analysis Consortium\r\n(DPAC, https://www.cosmos.esa.int/web/gaia/\r\ndpac/consortium).
  Funding for the DPAC has been\r\nprovided by national institutions, in particular
  the\r\ninstitutions participating in the Gaia Multilateral\r\nAgreement."
date_created: 2026-07-12T22:02:19Z
date_published: 2026-06-30T00:00:00Z
date_updated: 2026-07-13T09:09:34Z
day: '30'
ddc:
- '520'
department:
- _id: IlCa
doi: 10.33232/001c.164326
external_id:
  arxiv:
  - '2606.11293'
file:
- access_level: open_access
  checksum: 6320fd19e5ea3399f332be5aab022736
  content_type: application/pdf
  creator: dernst
  date_created: 2026-07-13T09:05:36Z
  date_updated: 2026-07-13T09:05:36Z
  file_id: '22282'
  file_name: 2026_OpenJourAstrophysics_ElBadry.pdf
  file_size: 1994596
  relation: main_file
  success: 1
file_date_updated: 2026-07-13T09:05:36Z
has_accepted_license: '1'
intvolume: '         9'
keyword:
- white dwarfs
- 'binaries: close'
- 'stars: chemically peculiar'
language:
- iso: eng
month: '06'
oa: 1
oa_version: Published Version
publication: The Open Journal of Astrophysics
publication_identifier:
  eissn:
  - 2565-6120
publication_status: published
publisher: Maynooth Academic Publishing
quality_controlled: '1'
researchdata_availability: no
scopus_import: '1'
status: public
supplementarymaterial: no
title: A systematic survey for hypervelocity runaways from thermonuclear supernovae
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 9
year: '2026'
...
---
OA_place: publisher
OA_type: hybrid
_id: '22269'
abstract:
- lang: eng
  text: The divisome apparatus synthesizes septal peptidoglycan (PG) during bacterial
    division. In Escherichia coli, the class A penicillin-binding protein (aPBP) called
    PBP1b has been implicated in division, but its role in the process has remained
    unclear. Here we show using in situ cryo-electron tomography, genetics and other
    imaging methods that PBP1b is required to produce a wedge-like density of PG at
    the division site and that loss of this structure weakens the division site, making
    it hypersusceptible to osmotic lysis. Surprisingly, the activator LpoB needed
    for general PBP1b function was not required for its role in division. Of the two
    PBP1b isoforms produced in cells, we show that the one with an extended cytoplasmic
    N terminus localizes to and functions at the division site, probably via recruitment
    by the FtsA component of the divisome. The conservation of aPBPs with extended
    cytoplasmic N termini suggests that other Gram-negative bacteria may use similar
    mechanisms for division site reinforcement.
acknowledgement: We thank all members of the Bernhardt, Rudner, Navarro and Vettiger
  Laboratories for support and helpful conversations. We thank C. Genoud, J. Daraspe,
  A. Mucciolo and D. de Bellis at the Electron Microscopy Facility of the University
  of Lausanne and E. Jeanvoine for providing access to workstations for cryo-ET image
  processing; S. Sterling, C. Borsa, J. Podgorski, P. Vinh Dip, E. Brignole and A.
  Osherov at the MIT.nano cryo-EM facility, K. Song and C. Xu at the University of
  Massachusetts cryo-EM facility, and R. Walsh and Z. Li at the cryo-EM at Harvard
  Medical School facility for providing access to the cryo-EM microscopes and for
  all their help, advice and maintenance of cryo-EM equipment. AFM was performed at
  the Harvard University Center for Nanoscale Systems (CNS), a member of the National
  Nanotechnology Coordinated Infrastructure Network (NNCI), which is supported by
  the National Science Foundation under NSF award no. ECCS-2025158. We thank N. S.
  Colella for excellent advice on AFM data acquisition and analysis; the MicRoN imaging
  core at Harvard Medical School for excellent advice on live cell imaging and maintenance
  of fluorescence microscopes; B. Krautz for creating the cartoon illustrations (www.sciencecommunicated.com);
  and L. Miles and R. Aeschimann for assistance with strain construction. A.V. was
  supported by an EMBO long-term postdoctoral fellowship ALTF_89-2019, the Swiss National
  Science Foundation (SNSF) Postdoc.Mobility fellowship P500PB_203143. P.P.N. was
  a recipient of early postdoc.mobility and postdoc.mobility fellowships (P2BSP3_188112
  and P400PB_199252). This work was also supported by funding from the National Institutes
  of Health (R35GM142553 to L.H.C. and R01AI083365 to T.G.B.), investigator funds
  from the Howard Hughes Medical Institute (T.G.B.), an SNSF project grant (320030-236243
  to A.V.), an SNSF Starting Grant (TMSGI3_218251 to P.P.N.), an SNSF Project grant
  (320030-236069 to P.P.N), an SNSF SPARK grant (CRSK-3_237167 to P.P.N.), cryo-EM
  funds from the Faculty of Biology and Medicine at University of Lausanne to P.P.N.
  and the Foundation Pierre Mercier pour la Science (to P.P.N.).
article_processing_charge: Yes (in subscription journal)
article_type: original
author:
- first_name: Paula P.
  full_name: Navarro, Paula P.
  last_name: Navarro
- first_name: Andrea
  full_name: Vettiger, Andrea
  last_name: Vettiger
- first_name: Roman
  full_name: Hajdu, Roman
  id: ffab949d-133f-11ed-8f02-94de21ace503
  last_name: Hajdu
- first_name: Virly Y.
  full_name: Ananda, Virly Y.
  last_name: Ananda
- first_name: Alejandro
  full_name: López-Tavares, Alejandro
  last_name: López-Tavares
- first_name: Ernst W.
  full_name: Schmid, Ernst W.
  last_name: Schmid
- first_name: Johannes C.
  full_name: Walter, Johannes C.
  last_name: Walter
- first_name: Martin
  full_name: Loose, Martin
  id: 462D4284-F248-11E8-B48F-1D18A9856A87
  last_name: Loose
  orcid: 0000-0001-7309-9724
- first_name: Luke H.
  full_name: Chao, Luke H.
  last_name: Chao
- first_name: Thomas G.
  full_name: Bernhardt, Thomas G.
  last_name: Bernhardt
citation:
  ama: Navarro PP, Vettiger A, Hajdu R, et al. The penicillin-binding protein PBP1b
    fortifies the Escherichia coli division site against osmotic rupture. <i>Nature
    Microbiology</i>. 2026. doi:<a href="https://doi.org/10.1038/s41564-026-02403-6">10.1038/s41564-026-02403-6</a>
  apa: Navarro, P. P., Vettiger, A., Hajdu, R., Ananda, V. Y., López-Tavares, A.,
    Schmid, E. W., … Bernhardt, T. G. (2026). The penicillin-binding protein PBP1b
    fortifies the Escherichia coli division site against osmotic rupture. <i>Nature
    Microbiology</i>. Springer Nature. <a href="https://doi.org/10.1038/s41564-026-02403-6">https://doi.org/10.1038/s41564-026-02403-6</a>
  chicago: Navarro, Paula P., Andrea Vettiger, Roman Hajdu, Virly Y. Ananda, Alejandro
    López-Tavares, Ernst W. Schmid, Johannes C. Walter, Martin Loose, Luke H. Chao,
    and Thomas G. Bernhardt. “The Penicillin-Binding Protein PBP1b Fortifies the Escherichia
    Coli Division Site against Osmotic Rupture.” <i>Nature Microbiology</i>. Springer
    Nature, 2026. <a href="https://doi.org/10.1038/s41564-026-02403-6">https://doi.org/10.1038/s41564-026-02403-6</a>.
  ieee: P. P. Navarro <i>et al.</i>, “The penicillin-binding protein PBP1b fortifies
    the Escherichia coli division site against osmotic rupture,” <i>Nature Microbiology</i>.
    Springer Nature, 2026.
  ista: Navarro PP, Vettiger A, Hajdu R, Ananda VY, López-Tavares A, Schmid EW, Walter
    JC, Loose M, Chao LH, Bernhardt TG. 2026. The penicillin-binding protein PBP1b
    fortifies the Escherichia coli division site against osmotic rupture. Nature Microbiology.
  mla: Navarro, Paula P., et al. “The Penicillin-Binding Protein PBP1b Fortifies the
    Escherichia Coli Division Site against Osmotic Rupture.” <i>Nature Microbiology</i>,
    Springer Nature, 2026, doi:<a href="https://doi.org/10.1038/s41564-026-02403-6">10.1038/s41564-026-02403-6</a>.
  short: P.P. Navarro, A. Vettiger, R. Hajdu, V.Y. Ananda, A. López-Tavares, E.W.
    Schmid, J.C. Walter, M. Loose, L.H. Chao, T.G. Bernhardt, Nature Microbiology
    (2026).
das_tickbox: '1'
dataavailabilitystatement: 'The data, plasmids and strains that support the findings
  of this study are available from the corresponding authors by request. Representative
  tomograms are deposited in EMDB: EMD-27479 (wild-type), EMD-53351 (∆ponB), EMD-53357(∆lpoB)
  and EMD-53363 (∆ponA). Corresponding raw movie frames and stacks of tilt series
  are deposited as EMPIAR-11090 (wild type), EMPIAR-13502 (∆ponB), EMPIAR-13513 (∆lpoB)
  and EMPIAR-13512 (∆ponA), and will be released upon publication. Other data related
  to this manuscript (for example, AFM, light microscopy, growth curves and so on)
  can be found on Zenodo at https://doi.org/10.5281/zenodo.20841819 (ref. 101). Source
  data are provided with this paper. Scripts used in this study were deposited on
  GitHub at https://github.com/NavarroVettiger/Navarro-et-al_2022 and https://github.com/virlyananda/EM-ImageProcessing.'
date_created: 2026-07-12T22:02:19Z
date_published: 2026-07-03T00:00:00Z
date_updated: 2026-07-13T09:22:49Z
day: '03'
ddc:
- '570'
department:
- _id: MaLo
- _id: GradSch
doi: 10.1038/s41564-026-02403-6
external_id:
  pmid:
  - '42399561'
has_accepted_license: '1'
language:
- iso: eng
main_file_link:
- open_access: '1'
  url: https://doi.org/10.1038/s41564-026-02403-6
month: '07'
oa: 1
oa_version: Published Version
pmid: 1
publication: Nature Microbiology
publication_identifier:
  eissn:
  - 2058-5276
publication_status: epub_ahead
publisher: Springer Nature
quality_controlled: '1'
researchdata_availability: yes
scopus_import: '1'
status: public
supplementarymaterial: yes
title: The penicillin-binding protein PBP1b fortifies the Escherichia coli division
  site against osmotic rupture
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '22288'
abstract:
- lang: eng
  text: Soft solids and their surface deformations control the response of many natural
    and artificial systems. Yet, their underlying properties are vigorously debated,
    particularly for polymer networks. While molecular-scale theories predict no interfacial
    changes with macroscopic deformation, multiple experiments suggest otherwise.
    To settle this issue, we measure displacement fields near the interface of a silicone
    gel, in the limit of small deformations. We discover an unexpected multiscale
    response. The shear modulus decreases smoothly by half with 20  μ⁢m of the interface.
    At the same time we observe a surface excess elasticity, that depends on history
    and outer medium composition. These results reveal the fundamentally multiscale
    nature of polymeric surfaces, and call for further experimental and theoretical
    investigations into the basic understanding of soft solid interfaces.
acknowledgement: The authors thank Katharine Jensen, Stefanie Heyden, Thomas Salez,
  Francesco Stellacci, Denis Bartolo, Francesco Picella, Hélène Delanoë-Ayari, Mathieu
  Leocmach, Antoine Bérut, Cécile Cottin-Bizonne, Anne-Laure Biance, and Oriane Talabart
  for useful discussions. We also thank the reviewers for excellent suggestions that
  substantively improved the manuscript.
article_number: '021063'
article_processing_charge: Yes
article_type: original
arxiv: 1
author:
- first_name: Nicolas
  full_name: Bain, Nicolas
  last_name: Bain
- first_name: Lawrence A.
  full_name: Wilen, Lawrence A.
  last_name: Wilen
- first_name: Dominic
  full_name: Gerber, Dominic
  last_name: Gerber
- first_name: Mengjie
  full_name: Zu, Mengjie
  id: 26dd9e7c-e86a-11eb-a854-82ac731c9ae2
  last_name: Zu
- first_name: Carl Peter
  full_name: Goodrich, Carl Peter
  id: EB352CD2-F68A-11E9-89C5-A432E6697425
  last_name: Goodrich
  orcid: 0000-0002-1307-5074
- first_name: Senthilkumar
  full_name: Duraivel, Senthilkumar
  last_name: Duraivel
- first_name: Kaarthik
  full_name: Varma, Kaarthik
  last_name: Varma
- first_name: Harsha
  full_name: Koganti, Harsha
  last_name: Koganti
- first_name: Robert W.
  full_name: Style, Robert W.
  last_name: Style
- first_name: Eric R.
  full_name: Dufresne, Eric R.
  last_name: Dufresne
citation:
  ama: Bain N, Wilen LA, Gerber D, et al. Multiscale interfacial mechanics of soft
    solids. <i>Physical Review X</i>. 2026;16(2). doi:<a href="https://doi.org/10.1103/8msx-l8s7">10.1103/8msx-l8s7</a>
  apa: Bain, N., Wilen, L. A., Gerber, D., Zu, M., Goodrich, C. P., Duraivel, S.,
    … Dufresne, E. R. (2026). Multiscale interfacial mechanics of soft solids. <i>Physical
    Review X</i>. American Physical Society. <a href="https://doi.org/10.1103/8msx-l8s7">https://doi.org/10.1103/8msx-l8s7</a>
  chicago: Bain, Nicolas, Lawrence A. Wilen, Dominic Gerber, Mengjie Zu, Carl Peter
    Goodrich, Senthilkumar Duraivel, Kaarthik Varma, Harsha Koganti, Robert W. Style,
    and Eric R. Dufresne. “Multiscale Interfacial Mechanics of Soft Solids.” <i>Physical
    Review X</i>. American Physical Society, 2026. <a href="https://doi.org/10.1103/8msx-l8s7">https://doi.org/10.1103/8msx-l8s7</a>.
  ieee: N. Bain <i>et al.</i>, “Multiscale interfacial mechanics of soft solids,”
    <i>Physical Review X</i>, vol. 16, no. 2. American Physical Society, 2026.
  ista: Bain N, Wilen LA, Gerber D, Zu M, Goodrich CP, Duraivel S, Varma K, Koganti
    H, Style RW, Dufresne ER. 2026. Multiscale interfacial mechanics of soft solids.
    Physical Review X. 16(2), 021063.
  mla: Bain, Nicolas, et al. “Multiscale Interfacial Mechanics of Soft Solids.” <i>Physical
    Review X</i>, vol. 16, no. 2, 021063, American Physical Society, 2026, doi:<a
    href="https://doi.org/10.1103/8msx-l8s7">10.1103/8msx-l8s7</a>.
  short: N. Bain, L.A. Wilen, D. Gerber, M. Zu, C.P. Goodrich, S. Duraivel, K. Varma,
    H. Koganti, R.W. Style, E.R. Dufresne, Physical Review X 16 (2026).
das_tickbox: '1'
dataavailabilitystatement: The data that support the findings of this article are
  openly available https://github.com/nicobain/Multiscale_interfacial_mechanics_soft_solids_data
date_created: 2026-07-13T09:40:54Z
date_published: 2026-06-30T00:00:00Z
date_updated: 2026-07-13T11:17:51Z
day: '30'
ddc:
- '530'
department:
- _id: CaGo
doi: 10.1103/8msx-l8s7
external_id:
  arxiv:
  - '2410.09158'
file:
- access_level: open_access
  checksum: 47354f40981223fb0c9afe292f16ead1
  content_type: application/pdf
  creator: dernst
  date_created: 2026-07-13T11:16:47Z
  date_updated: 2026-07-13T11:16:47Z
  file_id: '22309'
  file_name: 2026_PhysicalReviewX_Bain.pdf
  file_size: 4367284
  relation: main_file
  success: 1
file_date_updated: 2026-07-13T11:16:47Z
has_accepted_license: '1'
intvolume: '        16'
issue: '2'
language:
- iso: eng
month: '06'
oa: 1
oa_version: Published Version
publication: Physical Review X
publication_identifier:
  issn:
  - 2160-3308
publication_status: published
publisher: American Physical Society
quality_controlled: '1'
researchdata_availability: yes
scopus_import: '1'
status: public
supplementarymaterial: yes
title: Multiscale interfacial mechanics of soft solids
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 16
year: '2026'
...
---
OA_type: closed access
_id: '22286'
abstract:
- lang: eng
  text: Plants are remarkable organisms. Unlike animals, they cannot flee and, rooted
    in one place, they must cope with whatever challenges arise — nutrient scarcity,
    drought, shade, wind or obstacles in the soil. Their extraordinary ability to
    survive in such unstable environmental conditions lies in their capacity to adapt.
    In response to environmental signals, plants can rapidly adjust the rate of organ
    growth, change the direction of growth, bend toward resources, or remodel their
    body architecture by promoting or suppressing the formation of new organs such
    as lateral roots, branches, leaves, or flowers. This unique developmental plasticity
    depends on chemical signals, plant hormones that serve as regulators and coordinators
    of endogenous molecular and cellular processes. Chief among these signals is auxin,
    a plant hormone central to nearly every aspect of plant life.
article_processing_charge: No
article_type: original
author:
- first_name: Valentin
  full_name: Leitner, Valentin
  id: 4c665ce3-0016-11ec-bea0-e44de7a4fa3d
  last_name: Leitner
- first_name: Eva
  full_name: Benková, Eva
  id: 38F4F166-F248-11E8-B48F-1D18A9856A87
  last_name: Benková
  orcid: 0000-0002-8510-9739
citation:
  ama: Leitner V, Benková E. Auxin and the control of plant growth and development.
    <i>Current Biology</i>. 2026;36(13):R739-R744. doi:<a href="https://doi.org/10.1016/j.cub.2026.04.047">10.1016/j.cub.2026.04.047</a>
  apa: Leitner, V., &#38; Benková, E. (2026). Auxin and the control of plant growth
    and development. <i>Current Biology</i>. Elsevier. <a href="https://doi.org/10.1016/j.cub.2026.04.047">https://doi.org/10.1016/j.cub.2026.04.047</a>
  chicago: Leitner, Valentin, and Eva Benková. “Auxin and the Control of Plant Growth
    and Development.” <i>Current Biology</i>. Elsevier, 2026. <a href="https://doi.org/10.1016/j.cub.2026.04.047">https://doi.org/10.1016/j.cub.2026.04.047</a>.
  ieee: V. Leitner and E. Benková, “Auxin and the control of plant growth and development,”
    <i>Current Biology</i>, vol. 36, no. 13. Elsevier, pp. R739–R744, 2026.
  ista: Leitner V, Benková E. 2026. Auxin and the control of plant growth and development.
    Current Biology. 36(13), R739–R744.
  mla: Leitner, Valentin, and Eva Benková. “Auxin and the Control of Plant Growth
    and Development.” <i>Current Biology</i>, vol. 36, no. 13, Elsevier, 2026, pp.
    R739–44, doi:<a href="https://doi.org/10.1016/j.cub.2026.04.047">10.1016/j.cub.2026.04.047</a>.
  short: V. Leitner, E. Benková, Current Biology 36 (2026) R739–R744.
corr_author: '1'
das_tickbox: '0'
date_created: 2026-07-13T09:39:40Z
date_published: 2026-07-06T00:00:00Z
date_updated: 2026-07-13T11:11:56Z
day: '06'
department:
- _id: EvBe
- _id: GradSch
doi: 10.1016/j.cub.2026.04.047
external_id:
  pmid:
  - '42407441'
intvolume: '        36'
issue: '13'
language:
- iso: eng
month: '07'
oa_version: None
page: R739-R744
pmid: 1
publication: Current Biology
publication_identifier:
  issn:
  - 0960-9822
publication_status: published
publisher: Elsevier
quality_controlled: '1'
researchdata_availability: no
scopus_import: '1'
status: public
supplementarymaterial: no
title: Auxin and the control of plant growth and development
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 36
year: '2026'
...
---
OA_place: publisher
OA_type: hybrid
PlanS_conform: '1'
_id: '22291'
abstract:
- lang: eng
  text: Persistent homology is a fundamental tool in Topological Data Analysis. The
    associated algebraic structure is the persistence module, a sequence of vector
    spaces connected by linear maps. Persistence modules admit a complete and fast-to-compute
    invariant known as the persistence diagram. However, this is no longer the case
    for maps between persistence modules (i.e. persistence maps). We propose a new
    invariant for persistence maps, consisting of a partial matching between the persistence
    diagrams of the domain and codomain modules. We show that this invariant is additive
    with respect to the direct sum decomposition of persistence maps, is more discriminative
    than the image module, and is computable in cubic time. Furthermore, we provide
    an implementation and demonstrate its efficiency by integrating it with edge collapse
    techniques for flag complexes (e.g., Vietoris–Rips complexes). As a key technical
    contribution, we describe how to induce a persistence map between two flag complexes
    that have been independently simplified via edge collapses, even when a direct
    simplicial map between them is no longer available.
acknowledgement: This project was partially funded by MCIN/AEI and the NextGenerationEU/PRTR,
  under project TED2021-129438B-I00. The authors thank IMUS-Maria de Maeztu grant
  CEX2024-001517-M - Apoyo a Unidades de Excelencia María de Maeztu for supporting
  this research, funded by MICIU/AEI/ 10.13039/501100011033. The authors would also
  like to thank Lars M Salbu for fruitful discussions regarding the operators from
  Definition 4.1 and their relation with the order relations introduced in Definition
  3.2.
article_number: '102598'
article_processing_charge: No
article_type: original
arxiv: 1
author:
- first_name: Rocio
  full_name: Gonzalez-Diaz, Rocio
  last_name: Gonzalez-Diaz
- first_name: Manuel
  full_name: Soriano Trigueros, Manuel
  id: 15ebd7cf-15bf-11ee-aebd-bb4bb5121ea8
  last_name: Soriano Trigueros
  orcid: 0000-0003-2449-1433
- first_name: Alvaro
  full_name: Torras-Casas, Alvaro
  last_name: Torras-Casas
citation:
  ama: Gonzalez-Diaz R, Soriano Trigueros M, Torras-Casas A. Additive partial matchings
    induced by persistence maps. <i>Journal of Symbolic Computation</i>. 2026;138.
    doi:<a href="https://doi.org/10.1016/j.jsc.2026.102598">10.1016/j.jsc.2026.102598</a>
  apa: Gonzalez-Diaz, R., Soriano Trigueros, M., &#38; Torras-Casas, A. (2026). Additive
    partial matchings induced by persistence maps. <i>Journal of Symbolic Computation</i>.
    Elsevier. <a href="https://doi.org/10.1016/j.jsc.2026.102598">https://doi.org/10.1016/j.jsc.2026.102598</a>
  chicago: Gonzalez-Diaz, Rocio, Manuel Soriano Trigueros, and Alvaro Torras-Casas.
    “Additive Partial Matchings Induced by Persistence Maps.” <i>Journal of Symbolic
    Computation</i>. Elsevier, 2026. <a href="https://doi.org/10.1016/j.jsc.2026.102598">https://doi.org/10.1016/j.jsc.2026.102598</a>.
  ieee: R. Gonzalez-Diaz, M. Soriano Trigueros, and A. Torras-Casas, “Additive partial
    matchings induced by persistence maps,” <i>Journal of Symbolic Computation</i>,
    vol. 138. Elsevier, 2026.
  ista: Gonzalez-Diaz R, Soriano Trigueros M, Torras-Casas A. 2026. Additive partial
    matchings induced by persistence maps. Journal of Symbolic Computation. 138, 102598.
  mla: Gonzalez-Diaz, Rocio, et al. “Additive Partial Matchings Induced by Persistence
    Maps.” <i>Journal of Symbolic Computation</i>, vol. 138, 102598, Elsevier, 2026,
    doi:<a href="https://doi.org/10.1016/j.jsc.2026.102598">10.1016/j.jsc.2026.102598</a>.
  short: R. Gonzalez-Diaz, M. Soriano Trigueros, A. Torras-Casas, Journal of Symbolic
    Computation 138 (2026).
corr_author: '1'
das_tickbox: '1'
dataavailabilitystatement: The code used for the computational experiments is available
  in https://github.com/Cimagroup/IBloFunMatch
date_created: 2026-07-13T09:43:38Z
date_published: 2026-06-23T00:00:00Z
date_updated: 2026-07-13T12:00:07Z
day: '23'
ddc:
- '500'
department:
- _id: HeEd
doi: 10.1016/j.jsc.2026.102598
external_id:
  arxiv:
  - '2006.11100'
has_accepted_license: '1'
intvolume: '       138'
keyword:
- Persistence module
- Persistence map
- Persistent homology
language:
- iso: eng
main_file_link:
- open_access: '1'
  url: https://doi.org/10.1016/j.jsc.2026.102598
mathsc:
- 55N31
- 16G20
month: '06'
oa: 1
oa_version: Published Version
publication: Journal of Symbolic Computation
publication_identifier:
  eissn:
  - 1095-855X
  issn:
  - 0747-7171
publication_status: epub_ahead
publisher: Elsevier
quality_controlled: '1'
researchdata_availability: yes
scopus_import: '1'
status: public
supplementarymaterial: no
title: Additive partial matchings induced by persistence maps
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 138
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
_id: '22289'
abstract:
- lang: eng
  text: Single-stranded, helically folded aromatic oligoamides bearing anionic phosphonate
    side chains have been shown to bind to some DNA-binding proteins better than DNA
    itself. However, these DNA mimic foldamers have until now mainly consisted of
    a single repeat motif, like a poly(dA:dT) DNA duplex, and contained limited sequence
    information. Here, we introduce new monomers designed to display different chemical
    functionalities in the major groove of the DNA mimics. Four new Fmoc-protected
    amino acid monomers have been synthesized and incorporated into oligomers. Sixteen
    foldamer sequences were prepared on solid phase. Their conformations in solution
    and in the solid state and their conformational dynamics were investigated using
    nuclear magnetic resonance, circular dichroism, molecular modeling, and X-ray
    crystallography. The results show that three of the four new monomers behaved
    as designed and that their introduction enhances the conformational dynamics of
    the DNA mimic foldamers. In a fourth case, conformational behavior proved to be
    more complex than expected. The modified sequences retained the ability to bind
    to the bacterial histone-like protein HU. These results showcase design strategies
    to manipulate large molecular biomimetics in which not only side chains but also
    main chain components are varied. The new monomers pave the way to complex DNA
    mimic foldamer sequences targeting proteins that recognize sequence-selective
    DNA-binding proteins such as transcription factors or restriction enzymes.
acknowledgement: We acknowledge financial support from the European Research Council
  (ERC) under the European Union's Horizon Europe Framework Programme (grant agreement
  no. ERC-2021-ADG-320892) and from the China Scholarship Council (CSC, predoctoral
  fellowship to J. W.). We thank L. Allmendinger for assistance with NMR measurements,
  P. Mayer for his assistance in solving the crystal structures of 1 and 1d, L. Bodero
  for assistance with automated solid-phase synthesis, M. Rogovoi for providing monomer
  precursors, and M. Loos for the purification and analysis of compounds 15a–19a.
  We thank M. Soler-Lopez (ID23-1, ESRF, Grenoble) and I. Bento (EMBL P13, Petra III,
  DESY, Hamburg) for assistance during data collection at the synchrotron beamlines.
article_processing_charge: Yes
article_type: original
author:
- first_name: Jiaojiao
  full_name: Wu, Jiaojiao
  last_name: Wu
- first_name: Valentina
  full_name: Corvaglia, Valentina
  last_name: Corvaglia
- first_name: Tulika
  full_name: Chakrabortty, Tulika
  last_name: Chakrabortty
- first_name: Pradeep K
  full_name: Mandal, Pradeep K
  id: 6a3def15-d4b4-11ef-9fa9-a24c1f545ec3
  last_name: Mandal
  orcid: 0000-0001-5996-956X
- first_name: Ivan
  full_name: Huc, Ivan
  last_name: Huc
citation:
  ama: Wu J, Corvaglia V, Chakrabortty T, Mandal PK, Huc I. Tailoring the major groove
    of DNA mimic foldamers. <i>Chemical Science</i>. doi:<a href="https://doi.org/10.1039/d6sc00798h">10.1039/d6sc00798h</a>
  apa: Wu, J., Corvaglia, V., Chakrabortty, T., Mandal, P. K., &#38; Huc, I. (n.d.).
    Tailoring the major groove of DNA mimic foldamers. <i>Chemical Science</i>. Royal
    Society of Chemistry. <a href="https://doi.org/10.1039/d6sc00798h">https://doi.org/10.1039/d6sc00798h</a>
  chicago: Wu, Jiaojiao, Valentina Corvaglia, Tulika Chakrabortty, Pradeep K Mandal,
    and Ivan Huc. “Tailoring the Major Groove of DNA Mimic Foldamers.” <i>Chemical
    Science</i>. Royal Society of Chemistry, n.d. <a href="https://doi.org/10.1039/d6sc00798h">https://doi.org/10.1039/d6sc00798h</a>.
  ieee: J. Wu, V. Corvaglia, T. Chakrabortty, P. K. Mandal, and I. Huc, “Tailoring
    the major groove of DNA mimic foldamers,” <i>Chemical Science</i>. Royal Society
    of Chemistry.
  ista: Wu J, Corvaglia V, Chakrabortty T, Mandal PK, Huc I. Tailoring the major groove
    of DNA mimic foldamers. Chemical Science.
  mla: Wu, Jiaojiao, et al. “Tailoring the Major Groove of DNA Mimic Foldamers.” <i>Chemical
    Science</i>, Royal Society of Chemistry, doi:<a href="https://doi.org/10.1039/d6sc00798h">10.1039/d6sc00798h</a>.
  short: J. Wu, V. Corvaglia, T. Chakrabortty, P.K. Mandal, I. Huc, Chemical Science
    (n.d.).
das_tickbox: '1'
dataavailabilitystatement: "CCDC 2514117, 2514118, 2286782 and 2478322 (compound 1,
  compound 1d, oligomer 5, and oligomer 6, respectively) contain the supplementary
  crystallographic data for this paper.54a–d \r\n\r\nThe supporting data have been
  provided as part of the supplementary information (SI). Supplementary information:
  SI figures, detailed experimental protocols, crystallographic studies, and characterisation
  of new compounds. See DOI: https://doi.org/10.1039/d6sc00798h."
date_created: 2026-07-13T09:41:36Z
date_published: 2026-06-09T00:00:00Z
date_updated: 2026-07-13T11:24:29Z
day: '09'
ddc:
- '540'
department:
- _id: LifeSc
doi: 10.1039/d6sc00798h
has_accepted_license: '1'
language:
- iso: eng
month: '06'
oa_version: Published Version
publication: Chemical Science
publication_identifier:
  eissn:
  - 2041-6539
  issn:
  - 2041-6520
publication_status: inpress
publisher: Royal Society of Chemistry
quality_controlled: '1'
researchdata_availability: yes
scopus_import: '1'
status: public
supplementarymaterial: yes
title: Tailoring the major groove of DNA mimic foldamers
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
year: '2026'
...
---
OA_place: publisher
OA_type: hybrid
PlanS_conform: '1'
_id: '22290'
abstract:
- lang: eng
  text: We introduce a multi-band BCS free energy functional and prove that for a
    multi-band superconductor the effect of inter-band coupling can only increase
    the critical temperature, irrespective of its attractive or repulsive nature and
    its strength. Further, for weak coupling and weaker inter-band coupling, we prove
    that the dependence of the increase in critical temperature on the inter-band
    coupling is (1) linear, if there are two or more equally strongly superconducting
    bands, or (2) quadratic, if there is only one dominating band.
acknowledgement: 'We would like to thank J. Lenells and R. Seiringer for their interest
  and helpful discussions, E. Babaev and Y. Yerin for useful comments about the literature,
  and the anonymous referee for their comments. J.H. gratefully acknowledges partial
  financial support by the ERC Advanced Grant “RMTBeyond” No. 101020331 and the ERC
  Consollidator Grant “ProbQuant” (jointly with the Swiss State Secretariat for Education,
  Research and Innovation). E.L. gratefully acknowledges support from the Swedish
  Research Council, Grant No. 2023-04726. A.B.L. gratefully acknowledges partial financial
  support by the Austrian Science Fund (FWF) through grant DOI: 10.55776/I6427 (as
  part of the SFB/TRR 352) and by the French State support managed by ANR under the
  France 2030 program through the MaQuI CNRS Risky and High-Impact Research programme
  (RI)^2 (grant agreement ANR-24-RRII-0001). Open access funding provided by Royal
  Institute of Technology.'
article_processing_charge: Yes (via OA deal)
article_type: original
arxiv: 1
author:
- first_name: Sven Joscha
  full_name: Henheik, Sven Joscha
  id: 31d731d7-d235-11ea-ad11-b50331c8d7fb
  last_name: Henheik
  orcid: 0000-0003-1106-327X
- first_name: Edwin
  full_name: Langmann, Edwin
  last_name: Langmann
- first_name: Asbjørn Bækgaard
  full_name: Lauritsen, Asbjørn Bækgaard
  id: e1a2682f-dc8d-11ea-abe3-81da9ac728f1
  last_name: Lauritsen
  orcid: 0000-0003-4476-2288
citation:
  ama: Henheik SJ, Langmann E, Lauritsen AB. Multi-band superconductors have enhanced
    critical temperatures. <i>Annales Henri Poincaré</i>. 2026. doi:<a href="https://doi.org/10.1007/s00023-026-01706-y">10.1007/s00023-026-01706-y</a>
  apa: Henheik, S. J., Langmann, E., &#38; Lauritsen, A. B. (2026). Multi-band superconductors
    have enhanced critical temperatures. <i>Annales Henri Poincaré</i>. Springer Nature.
    <a href="https://doi.org/10.1007/s00023-026-01706-y">https://doi.org/10.1007/s00023-026-01706-y</a>
  chicago: Henheik, Sven Joscha, Edwin Langmann, and Asbjørn Bækgaard Lauritsen. “Multi-Band
    Superconductors Have Enhanced Critical Temperatures.” <i>Annales Henri Poincaré</i>.
    Springer Nature, 2026. <a href="https://doi.org/10.1007/s00023-026-01706-y">https://doi.org/10.1007/s00023-026-01706-y</a>.
  ieee: S. J. Henheik, E. Langmann, and A. B. Lauritsen, “Multi-band superconductors
    have enhanced critical temperatures,” <i>Annales Henri Poincaré</i>. Springer
    Nature, 2026.
  ista: Henheik SJ, Langmann E, Lauritsen AB. 2026. Multi-band superconductors have
    enhanced critical temperatures. Annales Henri Poincaré.
  mla: Henheik, Sven Joscha, et al. “Multi-Band Superconductors Have Enhanced Critical
    Temperatures.” <i>Annales Henri Poincaré</i>, Springer Nature, 2026, doi:<a href="https://doi.org/10.1007/s00023-026-01706-y">10.1007/s00023-026-01706-y</a>.
  short: S.J. Henheik, E. Langmann, A.B. Lauritsen, Annales Henri Poincaré (2026).
das_tickbox: '1'
dataavailabilitystatement: Data sharing is not applicable to this article as no new
  data were created or analyzed in this study.
date_created: 2026-07-13T09:42:22Z
date_published: 2026-06-29T00:00:00Z
date_updated: 2026-07-13T11:34:08Z
day: '29'
ddc:
- '500'
department:
- _id: LaEr
- _id: RoSe
doi: 10.1007/s00023-026-01706-y
ec_funded: 1
external_id:
  arxiv:
  - '2409.17297'
has_accepted_license: '1'
language:
- iso: eng
main_file_link:
- open_access: '1'
  url: https://doi.org/10.1007/s00023-026-01706-y
month: '06'
oa: 1
oa_version: Published Version
project:
- _id: 62796744-2b32-11ec-9570-940b20777f1d
  call_identifier: H2020
  grant_number: '101020331'
  name: Random matrices beyond Wigner-Dyson-Mehta
- _id: bda63fe5-d553-11ed-ba76-a16e3d2f256b
  grant_number: I06427
  name: Mathematical Challenges in BCS Theory of Superconductivity
publication: Annales Henri Poincaré
publication_identifier:
  eissn:
  - 1424-0661
  issn:
  - 1424-0637
publication_status: epub_ahead
publisher: Springer Nature
quality_controlled: '1'
related_material:
  record:
  - id: '19550'
    relation: earlier_version
    status: public
researchdata_availability: not applicable
scopus_import: '1'
status: public
supplementarymaterial: not applicable
title: Multi-band superconductors have enhanced critical temperatures
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
year: '2026'
...
---
OA_place: repository
OA_type: green
_id: '22292'
abstract:
- lang: eng
  text: We show that a suitable choice of boundary conditions for the Laplacian allows
    for the appearance of an arbitrary number of condensates, described by arbitrary
    harmonic functions, in the thermodynamic limit of an ideal Bose gas.
acknowledgement: We are grateful to Rupert Frank and Jakob Yngvason for helpful discussions
  and suggestions.
article_number: '061901'
article_processing_charge: No
article_type: original
arxiv: 1
author:
- first_name: Michiel
  full_name: De Wilde, Michiel
  id: bebf1407-6635-11f0-9fef-9b7e2dd151d0
  last_name: De Wilde
- first_name: Robert
  full_name: Seiringer, Robert
  id: 4AFD0470-F248-11E8-B48F-1D18A9856A87
  last_name: Seiringer
  orcid: 0000-0002-6781-0521
citation:
  ama: De Wilde M, Seiringer R. Arbitrary harmonic functions as Bose–Einstein condensates.
    <i>Journal of Mathematical Physics</i>. 2026;67(6). doi:<a href="https://doi.org/10.1063/5.0325354">10.1063/5.0325354</a>
  apa: De Wilde, M., &#38; Seiringer, R. (2026). Arbitrary harmonic functions as Bose–Einstein
    condensates. <i>Journal of Mathematical Physics</i>. AIP Publishing. <a href="https://doi.org/10.1063/5.0325354">https://doi.org/10.1063/5.0325354</a>
  chicago: De Wilde, Michiel, and Robert Seiringer. “Arbitrary Harmonic Functions
    as Bose–Einstein Condensates.” <i>Journal of Mathematical Physics</i>. AIP Publishing,
    2026. <a href="https://doi.org/10.1063/5.0325354">https://doi.org/10.1063/5.0325354</a>.
  ieee: M. De Wilde and R. Seiringer, “Arbitrary harmonic functions as Bose–Einstein
    condensates,” <i>Journal of Mathematical Physics</i>, vol. 67, no. 6. AIP Publishing,
    2026.
  ista: De Wilde M, Seiringer R. 2026. Arbitrary harmonic functions as Bose–Einstein
    condensates. Journal of Mathematical Physics. 67(6), 061901.
  mla: De Wilde, Michiel, and Robert Seiringer. “Arbitrary Harmonic Functions as Bose–Einstein
    Condensates.” <i>Journal of Mathematical Physics</i>, vol. 67, no. 6, 061901,
    AIP Publishing, 2026, doi:<a href="https://doi.org/10.1063/5.0325354">10.1063/5.0325354</a>.
  short: M. De Wilde, R. Seiringer, Journal of Mathematical Physics 67 (2026).
corr_author: '1'
das_tickbox: '1'
dataavailabilitystatement: Data sharing is not applicable to this article as no new
  data were created or analyzed in this study.
date_created: 2026-07-13T09:45:09Z
date_published: 2026-06-01T00:00:00Z
date_updated: 2026-07-13T12:20:59Z
day: '01'
department:
- _id: RoSe
- _id: GradSch
doi: 10.1063/5.0325354
external_id:
  arxiv:
  - '2601.22883'
intvolume: '        67'
issue: '6'
language:
- iso: eng
main_file_link:
- open_access: '1'
  url: https://doi.org/10.48550/arXiv.2601.22883
month: '06'
oa: 1
oa_version: Preprint
publication: Journal of Mathematical Physics
publication_identifier:
  eissn:
  - 1089-7658
  issn:
  - 0022-2488
publication_status: published
publisher: AIP Publishing
quality_controlled: '1'
researchdata_availability: not applicable
scopus_import: '1'
status: public
supplementarymaterial: not applicable
title: Arbitrary harmonic functions as Bose–Einstein condensates
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 67
year: '2026'
...
---
OA_type: closed access
_id: '22293'
abstract:
- lang: eng
  text: In order to cope with arid terrestrial environments, angiosperms have evolved
    a unique fertilization way—siphonogamy. The success of siphonogamy requires several
    prerequisites, including the normal development of the female gametophyte and
    male gametophyte (pollen). Appropriate pollination methods ensure the successful
    encounter between pollen and the stigma. After pollen lands on the stigma, pollen/pollen
    tube interacts with different tissues and cells of the pistil, completing a series
    of male-female communications. The smooth progress of these interactions ensures
    that the pollen tube can enter the female gametophyte, burst, and release sperm
    cells to complete the double fertilization. In this chapter, we provide an overview
    of pollination and the interactions between male and female, comprehensively summarizing
    the factors involved in these processes.
article_processing_charge: No
author:
- first_name: Sheng
  full_name: Zhong, Sheng
  last_name: Zhong
- first_name: Zijun
  full_name: Lan, Zijun
  last_name: Lan
- first_name: Zengxiang
  full_name: Ge, Zengxiang
  id: f43371a3-09ff-11eb-8013-bd0c6a2f6de8
  last_name: Ge
  orcid: 0000-0001-9381-3577
- first_name: Li-Jia
  full_name: Qu, Li-Jia
  last_name: Qu
citation:
  ama: 'Zhong S, Lan Z, Ge Z, Qu L-J. Pollination and Fertilization. In: Chang F,
    Wang Y, Ma H, eds. <i>Regulation of Plant Development</i>. Singapore: Springer
    Nature; 2026:537-615. doi:<a href="https://doi.org/10.1007/978-981-95-7033-1_14">10.1007/978-981-95-7033-1_14</a>'
  apa: 'Zhong, S., Lan, Z., Ge, Z., &#38; Qu, L.-J. (2026). Pollination and Fertilization.
    In F. Chang, Y. Wang, &#38; H. Ma (Eds.), <i>Regulation of Plant Development</i>
    (pp. 537–615). Singapore: Springer Nature. <a href="https://doi.org/10.1007/978-981-95-7033-1_14">https://doi.org/10.1007/978-981-95-7033-1_14</a>'
  chicago: 'Zhong, Sheng, Zijun Lan, Zengxiang Ge, and Li-Jia Qu. “Pollination and
    Fertilization.” In <i>Regulation of Plant Development</i>, edited by Fang  Chang,
    Yingxiang Wang, and Hong Ma, 537–615. Singapore: Springer Nature, 2026. <a href="https://doi.org/10.1007/978-981-95-7033-1_14">https://doi.org/10.1007/978-981-95-7033-1_14</a>.'
  ieee: 'S. Zhong, Z. Lan, Z. Ge, and L.-J. Qu, “Pollination and Fertilization,” in
    <i>Regulation of Plant Development</i>, F. Chang, Y. Wang, and H. Ma, Eds. Singapore:
    Springer Nature, 2026, pp. 537–615.'
  ista: 'Zhong S, Lan Z, Ge Z, Qu L-J. 2026.Pollination and Fertilization. In: Regulation
    of Plant Development. , 537–615.'
  mla: Zhong, Sheng, et al. “Pollination and Fertilization.” <i>Regulation of Plant
    Development</i>, edited by Fang  Chang et al., Springer Nature, 2026, pp. 537–615,
    doi:<a href="https://doi.org/10.1007/978-981-95-7033-1_14">10.1007/978-981-95-7033-1_14</a>.
  short: S. Zhong, Z. Lan, Z. Ge, L.-J. Qu, in:, F. Chang, Y. Wang, H. Ma (Eds.),
    Regulation of Plant Development, Springer Nature, Singapore, 2026, pp. 537–615.
das_tickbox: '1'
date_created: 2026-07-13T09:46:18Z
date_published: 2026-04-24T00:00:00Z
date_updated: 2026-07-13T12:25:19Z
day: '24'
department:
- _id: JiFr
doi: 10.1007/978-981-95-7033-1_14
editor:
- first_name: 'Fang '
  full_name: 'Chang, Fang '
  last_name: Chang
- first_name: Yingxiang
  full_name: Wang, Yingxiang
  last_name: Wang
- first_name: Hong
  full_name: Ma, Hong
  last_name: Ma
language:
- iso: eng
month: '04'
oa_version: None
page: 537-615
place: Singapore
publication: Regulation of Plant Development
publication_identifier:
  eisbn:
  - '9789819570331'
  isbn:
  - '9789819570324'
publication_status: published
publisher: Springer Nature
quality_controlled: '1'
scopus_import: '1'
status: public
title: Pollination and Fertilization
type: book_chapter
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
year: '2026'
...
---
OA_place: publisher
OA_type: hybrid
PlanS_conform: '1'
_id: '21378'
abstract:
- lang: eng
  text: From insects to mammals, essential brain functions, such as forming long-term
    memories (LTMs), increase metabolic activity in stimulated neurons to meet the
    energetic demand associated with brain activation. However, while impairing neuronal
    metabolism limits brain performance, whether expanding the metabolic capacity
    of neurons boosts brain function remains poorly understood. Here, we show that
    LTM formation of flies and mice can be enhanced by increasing mitochondrial metabolism
    in central memory circuits. By knocking down the mitochondrial Ca2+ exporter Letm1,
    we favour Ca2+ retention in the mitochondrial matrix of neurons due to reduction
    of mitochondrial H+/Ca2+ exchange. The resulting increase in mitochondrial Ca2+
    over-activates mitochondrial metabolism in neurons of central memory circuits,
    leading to improved LTM storage in training paradigms in which wild-type counterparts
    of both species fail to remember. Our findings unveil an evolutionarily conserved
    mechanism that controls mitochondrial metabolism in neurons and indicate its involvement
    in shaping higher brain functions, such as LTM.
acknowledgement: We thank all members of the laboratory of J.d.J.-S. for insightful
  discussions and comments. We thank S. Perez for technical assistance. This work
  was made possible by the Paris Brain Institute Diane Barriere Chair in Synaptic
  Bioenergetics awarded to J.d.J.-S., who is also supported by an ERC Starting Grant
  (SynaptoEnergy, European Research Council; ERC-StG-852873), 2019 ATIP-Avenir Grant
  (CNRS, Inserm), a Big Brain Theory Grant (ICM Foundation) and a Kavli Exploratory
  Award (Kavli Foundation). This work was also supported by an ERC Advanced Grant
  (EnergyMeMo; ERC-AdG-741550) to T.P. and grants from the Agence Nationale de la
  Recherche to P.Y.P. (ANR-20-CE92-0047-01), T.P. (ANR-23-CE16-0029-01), A.P. and
  J.d.J.-S. (ANR-22-CE16-0020) and J.d.J.-S. (ANR-24-CE16-0221). T.P., P.Y.P. and
  J.d.J.-S. are permanent CNRS researchers. A.P. is a permanent ESPCI associate professor.
  T.C. was funded by the French Ministry of Research and the Fondation pour la Recherche
  Médicale. V.R. was funded by the Max Planck Society, the Chan Zuckerberg Initiative
  DAF, an advised fund of the Silicon Valley Community Foundation grant number 2024-349543
  and the NIH Director’s New Innovator Award (DP2 MH140148). A.B.-G. and C.R.-D. received
  funding from an ERC Starting Grant (HighMemory; ERC-StG-948217), the Ministry of
  Economy and Competitiveness (PID2021-122795OB-I00) and the Departament d’Economia
  i Coneixement de la Generalitat de Catalunya (SGR 00022). T.P.V. was funded by the
  Wellcome Trust and a Royal Society Sir Henry Dale Research Fellowship (WT100000)
  and a Wellcome Trust Senior Research Fellowship (214316/Z/18/Z). K.G. was supported
  by the DIM C-BRAINS, funded by the Conseil Régional d’Ile-de-France. The contributions
  of H.F. and E.R.S. were supported by the Howard Hughes Medical Institute. The PHENO-ICMice
  animal Core at ICM is supported by two ‘Investissements d’avenir’ (ANR-10- IAIHU-06
  and ANR-11-INBS-0011-NeurATRIS) and the Fondation pour la Recherche Médicale.
article_processing_charge: Yes (in subscription journal)
article_type: original
author:
- first_name: Anjali
  full_name: Amrapali Vishwanath, Anjali
  last_name: Amrapali Vishwanath
- first_name: Typhaine
  full_name: Comyn, Typhaine
  last_name: Comyn
- first_name: Rodrigo G.
  full_name: Mira, Rodrigo G.
  last_name: Mira
- first_name: Claire
  full_name: Brossier, Claire
  last_name: Brossier
- first_name: Carlos
  full_name: Pascual-Caro, Carlos
  last_name: Pascual-Caro
- first_name: Maya
  full_name: Faour, Maya
  last_name: Faour
- first_name: Kahina
  full_name: Boumendil, Kahina
  last_name: Boumendil
- first_name: Chaitanya
  full_name: Chintaluri, Chaitanya
  id: BA06AFEE-A4BA-11EA-AE5C-14673DDC885E
  last_name: Chintaluri
  orcid: 0000-0003-4252-1608
- first_name: Carla
  full_name: Ramon-Duaso, Carla
  last_name: Ramon-Duaso
- first_name: Ruolin
  full_name: Fan, Ruolin
  last_name: Fan
- first_name: Kishalay
  full_name: Ghosh, Kishalay
  last_name: Ghosh
- first_name: Helen
  full_name: Farrants, Helen
  last_name: Farrants
- first_name: Jean-Paul
  full_name: Berwick, Jean-Paul
  last_name: Berwick
- first_name: Riya
  full_name: Sivakumar, Riya
  last_name: Sivakumar
- first_name: Mario
  full_name: Lopez-Manzaneda, Mario
  last_name: Lopez-Manzaneda
- first_name: Eric R.
  full_name: Schreiter, Eric R.
  last_name: Schreiter
- first_name: Thomas
  full_name: Preat, Thomas
  last_name: Preat
- first_name: Tim P
  full_name: Vogels, Tim P
  id: CB6FF8D2-008F-11EA-8E08-2637E6697425
  last_name: Vogels
  orcid: 0000-0003-3295-6181
- first_name: Vidhya
  full_name: Rangaraju, Vidhya
  last_name: Rangaraju
- first_name: Arnau
  full_name: Busquets-Garcia, Arnau
  last_name: Busquets-Garcia
- first_name: Pierre-Yves
  full_name: Plaçais, Pierre-Yves
  last_name: Plaçais
- first_name: Alice
  full_name: Pavlowsky, Alice
  last_name: Pavlowsky
- first_name: Jaime
  full_name: de Juan-Sanz, Jaime
  last_name: de Juan-Sanz
citation:
  ama: Amrapali Vishwanath A, Comyn T, Mira RG, et al. Mitochondrial Ca2+ efflux controls
    neuronal metabolism and long-term memory across species. <i>Nature Metabolism</i>.
    2026;8(2):467-488. doi:<a href="https://doi.org/10.1038/s42255-026-01451-w">10.1038/s42255-026-01451-w</a>
  apa: Amrapali Vishwanath, A., Comyn, T., Mira, R. G., Brossier, C., Pascual-Caro,
    C., Faour, M., … de Juan-Sanz, J. (2026). Mitochondrial Ca2+ efflux controls neuronal
    metabolism and long-term memory across species. <i>Nature Metabolism</i>. Springer
    Nature. <a href="https://doi.org/10.1038/s42255-026-01451-w">https://doi.org/10.1038/s42255-026-01451-w</a>
  chicago: Amrapali Vishwanath, Anjali, Typhaine Comyn, Rodrigo G. Mira, Claire Brossier,
    Carlos Pascual-Caro, Maya Faour, Kahina Boumendil, et al. “Mitochondrial Ca2+
    Efflux Controls Neuronal Metabolism and Long-Term Memory across Species.” <i>Nature
    Metabolism</i>. Springer Nature, 2026. <a href="https://doi.org/10.1038/s42255-026-01451-w">https://doi.org/10.1038/s42255-026-01451-w</a>.
  ieee: A. Amrapali Vishwanath <i>et al.</i>, “Mitochondrial Ca2+ efflux controls
    neuronal metabolism and long-term memory across species,” <i>Nature Metabolism</i>,
    vol. 8, no. 2. Springer Nature, pp. 467–488, 2026.
  ista: Amrapali Vishwanath A, Comyn T, Mira RG, Brossier C, Pascual-Caro C, Faour
    M, Boumendil K, Chintaluri C, Ramon-Duaso C, Fan R, Ghosh K, Farrants H, Berwick
    J-P, Sivakumar R, Lopez-Manzaneda M, Schreiter ER, Preat T, Vogels TP, Rangaraju
    V, Busquets-Garcia A, Plaçais P-Y, Pavlowsky A, de Juan-Sanz J. 2026. Mitochondrial
    Ca2+ efflux controls neuronal metabolism and long-term memory across species.
    Nature Metabolism. 8(2), 467–488.
  mla: Amrapali Vishwanath, Anjali, et al. “Mitochondrial Ca2+ Efflux Controls Neuronal
    Metabolism and Long-Term Memory across Species.” <i>Nature Metabolism</i>, vol.
    8, no. 2, Springer Nature, 2026, pp. 467–88, doi:<a href="https://doi.org/10.1038/s42255-026-01451-w">10.1038/s42255-026-01451-w</a>.
  short: A. Amrapali Vishwanath, T. Comyn, R.G. Mira, C. Brossier, C. Pascual-Caro,
    M. Faour, K. Boumendil, C. Chintaluri, C. Ramon-Duaso, R. Fan, K. Ghosh, H. Farrants,
    J.-P. Berwick, R. Sivakumar, M. Lopez-Manzaneda, E.R. Schreiter, T. Preat, T.P.
    Vogels, V. Rangaraju, A. Busquets-Garcia, P.-Y. Plaçais, A. Pavlowsky, J. de Juan-Sanz,
    Nature Metabolism 8 (2026) 467–488.
das_tickbox: '1'
date_created: 2026-03-02T10:04:49Z
date_published: 2026-02-11T00:00:00Z
date_updated: 2026-07-13T12:30:14Z
day: '11'
ddc:
- '570'
department:
- _id: TiVo
doi: 10.1038/s42255-026-01451-w
external_id:
  pmid:
  - '41673453'
file:
- access_level: open_access
  checksum: 365932a599d05bc9ce8a57204e7a1465
  content_type: application/pdf
  creator: dernst
  date_created: 2026-03-02T15:21:27Z
  date_updated: 2026-03-02T15:21:27Z
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  file_name: 2026_NatureMetab_AmrapaliVishwanath.pdf
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has_accepted_license: '1'
intvolume: '         8'
issue: '2'
language:
- iso: eng
month: '02'
oa: 1
oa_version: Published Version
page: 467-488
pmid: 1
project:
- _id: c084a126-5a5b-11eb-8a69-d75314a70a87
  grant_number: 214316/Z/18/Z
  name: What’s in a memory? Spatiotemporal dynamics in strongly coupled recurrent
    neuronal networks.
publication: Nature Metabolism
publication_identifier:
  eissn:
  - 2522-5812
publication_status: published
publisher: Springer Nature
quality_controlled: '1'
scopus_import: '1'
status: public
title: Mitochondrial Ca2+ efflux controls neuronal metabolism and long-term memory
  across species
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 8
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
_id: '22296'
abstract:
- lang: eng
  text: 'The detection of strong Balmer breaks and absorption features in Little Red
    Dots (LRDs) suggests they host active galactic nuclei embedded within dense gas
    envelopes, potentially powered by super-Eddington accretion. We present GLIMPSE-17775,
    a luminous (Lbol ∼ 1045 erg s−1) LRD at z = 3.501 behind Abell S1063 (μ ∼ 2),
    observed with deep JWST/NIRCam and a ∼20 hr (80 hr delensed) NIRSpec G395M spectrum.
    The data reveal over 40 emission and absorption features, including a rich forest
    of low-ionization Fe ii lines and numerous broad hydrogen recombination transitions.
    We use this depth to test the dense-gas interpretation through five independent
    diagnostics. Nearly all permitted lines show exponential wings with consistent
    FWHM, a signature of Thomson scattering requiring ne ≳ 108 cm−3. Adopting this
    width yields MBH ∼ 106.7M⊙, a factor of 10 lower than Gaussian fits, and λEdd
    ∼ 1.8. Additional diagnostics support the same picture: a pronounced Balmer break
    (fν,4050/fν,3670 = 2.0 ± 0.1), enhanced He i λ7065 and λ10830 with P-Cygni absorption,
    Bowen-fluorescent O i λ8446–λ11290 emission requiring Lyβ pumping, and 16 Fe ii
    lines matching fluorescence models. These features indicate a dense (n ∼ 108 cm−3),
    partially ionized cocoon where scattering and fluorescence dominate line formation,
    providing strong evidence that at least some LRDs are powered by super-Eddington
    black hole growth in the early Universe.'
acknowledgement: "IOP Science home\r\nThe Astrophysical Journal\r\nThe American Astronomical
  Society, find out more.\r\n\r\nThe following article isOpen access\r\nThe Deepest
  GLIMPSE of a Dense Gas Cocoon Enshrouding a Little Red Dot\r\nVasily Kokorev, John
  Chisholm, Rohan P. Naidu, Seiji Fujimoto, Hakim Atek, Gabriel Brammer, Steven L.
  Finkelstein, Hollis B. Akins, Danielle A. Berg, Lukas J. FurtakShow full author
  list\r\n\r\nPublished 2026 June 10 • © 2026. The Author(s). Published by the American
  Astronomical Society.\r\nThe Astrophysical Journal, Volume 1004, Number 2\r\nCitation
  Vasily Kokorev et al 2026 ApJ 1004 153\r\nDOI 10.3847/1538-4357/ae4ed7\r\n\r\nPDFOpens
  in a new tab.ePub\r\nAuthors\r\nFigures\r\nTables\r\nReferences\r\nArticle data\r\nPDFOpens
  in a new tab.ePub\r\nArticle metrics\r\n5138 Total downloads\r\n\r\n22 total citations
  on Dimensions.\r\nShare this article\r\nArticle information\r\nAbstract\r\nThe detection
  of strong Balmer breaks and absorption features in Little Red Dots (LRDs) suggests
  they host active galactic nuclei embedded within dense gas envelopes, potentially
  powered by super-Eddington accretion. We present GLIMPSE-17775, a luminous (Lbol
  ∼ 1045 erg s−1) LRD at z = 3.501 behind Abell S1063 (μ ∼ 2), observed with deep
  JWST/NIRCam and a ∼20 hr (80 hr delensed) NIRSpec G395M spectrum. The data reveal
  over 40 emission and absorption features, including a rich forest of low-ionization
  Fe ii lines and numerous broad hydrogen recombination transitions. We use this depth
  to test the dense-gas interpretation through five independent diagnostics. Nearly
  all permitted lines show exponential wings with consistent FWHM, a signature of
  Thomson scattering requiring ne ≳ 108 cm−3. Adopting this width yields MBH ∼ 106.7M⊙,
  a factor of 10 lower than Gaussian fits, and λEdd ∼ 1.8. Additional diagnostics
  support the same picture: a pronounced Balmer break (fν,4050/fν,3670 = 2.0 ± 0.1),
  enhanced He i λ7065 and λ10830 with P-Cygni absorption, Bowen-fluorescent O i λ8446–λ11290
  emission requiring Lyβ pumping, and 16 Fe ii lines matching fluorescence models.
  These features indicate a dense (n ∼ 108 cm−3), partially ionized cocoon where scattering
  and fluorescence dominate line formation, providing strong evidence that at least
  some LRDs are powered by super-Eddington black hole growth in the early Universe.\r\n\r\nExport
  citation and abstract\r\nBibTeXRIS\r\n\r\nPrevious article in issue\r\nNext article
  in issue\r\nRelated links\r\n\r\nOriginal content from this work may be used under
  the terms of the Creative Commons Attribution 4.0 licence. Any further distribution
  of this work must maintain attribution to the author(s) and the title of the work,
  journal citation and DOI.\r\n\r\n1. Introduction\r\nOne of the most enticing puzzles
  brought about by the launch of the James Webb Space Telescope (JWST) has been the
  discovery of red, compact objects called “Little Red Dots” (LRDs; J. Matthee et
  al. 2024). Previously invisible to the Hubble Space Telescope (HST) due to their
  extreme faintness in the optical and lack of near-infrared (NIR) coverage, LRDs
  have emerged in abundance (V. Kokorev et al. 2024a; H. B. Akins et al. 2025a; D.
  D. Kocevski et al. 2025; G. Barro et al. 2026) thanks to the unprecedented NIR sensitivity
  of JWST.\r\n\r\nTheir unusual properties—such as compact morphologies in rest-optical
  and distinctive “V-shaped” spectral energy distributions (SEDs)—make LRDs easy to
  identify in JWST fields; however, this is where the simplicity ends. Explaining
  LRDs as either evolved or dusty compact galaxies proves difficult: The former scenario
  requires massive stellar populations that strain Lambda cold dark matter (ΛCDM)
  predictions (M. Boylan-Kolchin 2023; I. Labbé et al. 2023), while the latter implies
  significant dust emission, yet none is observed (C. M. Casey et al. 2024; G. C.
  K. Leung et al. 2025; H. B. Akins et al. 2025a; I. Labbé et al. 2025).\r\n\r\nOver
  time, the accumulating detections of broad Balmer-series emission lines (D. D. Kocevski
  et al. 2023, 2025; J. Matthee et al. 2024, just to name a few), often accompanied
  by signatures of extreme ionization (e.g., V. Kokorev et al. 2023), have begun to
  clarify the physical origin of LRDs, pointing increasingly toward active galactic
  nuclei (AGN) as the underlying power source. In parallel, the much needed advent
  of NIRSpec Micro Shutter Assembly (MSA) programs based on red targets selected from
  JWST imaging (e.g., A. de Graaff et al. 2025b) has provided critical confirmation:
  Nearly all point sources exhibiting “V-shaped” SEDs reveal broad emission lines
  upon spectroscopic follow-up (R. E. Hviding et al. 2025), solidifying their AGN
  interpretation.\r\n\r\nThe nature of the spectral inflection point in LRDs, typically
  located near ∼3600 Å, has also undergone significant revision. Initially interpreted
  as a stellar Balmer break (I. Labbé et al. 2023), this feature implied implausibly
  high stellar masses (M*) far too early in cosmic history (M. Boylan-Kolchin 2023;
  N. Sabti et al. 2024). A second hypothesis invoked differential dust attenuation
  and host-galaxy contamination in the rest-UV to explain the sharp discontinuity
  (M. Volonteri et al. 2025). However, this explanation was soon ruled out by D. J.
  Setton et al. (2025) and Y. Ma et al. (2025), who demonstrated that the break generally
  lies around the Balmer limit, albeit with a fundamentally different origin than
  initially proposed.\r\n\r\nMore recently, a series of theoretical and observational
  works have converged on a new picture in which LRDs may host accreting black holes
  enshrouded in exceptionally dense, partially ionized gas cocoons, often referred
  to as “black hole stars” (hereafter BH*; A. de Graaff et al. 2025b; K. Inayoshi
  & R. Maiolino 2025; R. P. Naidu et al. 2025; A. J. Taylor et al. 2025). Here, BH*
  is used in an empirical sense to denote cocooned black holes whose emergent spectra
  exhibit a combination of black-hole-like and star-like features, such as broad permitted
  lines, steep Balmer-limit breaks, and Balmer absorption, as observed in the archetypal
  BH* sources (A. de Graaff et al. 2025b; R. P. Naidu et al. 2025). This usage does
  not assume a specific geometry or formation channel: The underlying physical picture
  involves an AGN power-law ionizing spectrum processed through very dense gas, and
  similar phenomenology can arise in a range of dense-gas configurations (e.g., K.
  Inayoshi & R. Maiolino 2025; D. Kido et al. 2025; H. Liu et al. 2025; A. Sneppen
  et al. 2026). In such environments, suppressed X-ray and radio emission (e.g., K.
  Inayoshi & R. Maiolino 2025; R. P. Naidu et al. 2025) arise naturally from the high
  optical depth, while the UV emission and forbidden optical lines (e.g., [O iii]
  λλ4959, 5007) may originate in the more extended host (e.g., A. de Graaff et al.
  2025d).\r\n\r\nThe dense-gas interpretation also offers a natural explanation for
  the P-Cygni-like Balmer and helium profiles frequently seen in high-signal-to-noise-ratio
  (S/N) spectra (J. Matthee et al. 2024), the non-Gaussian, exponentially winged line
  shapes predicted by radiative-transfer models of scattering in ionized gas (S.-J.
  Chang et al. 2026; V. Rusakov et al. 2026), and Lyα-like resonantly scattered shapes
  (R. P. Naidu et al. 2025; S.-J. Chang et al. 2026). Intriguingly, if electron and
  resonant scattering indeed dominate the broad-line widths, then the true virial
  velocities (traced by intrinsically narrower Gaussian cores)—and hence black hole
  masses—could be lower by an order of magnitude, alleviating the apparent tension
  between LRD black hole masses and their compact host galaxies (V. Rusakov et al.
  2026).\r\n\r\nSo far, however, the BH*/dense-gas interpretation of LRDs has relied
  largely on the Balmer break, occasional absorption features (X. Lin et al. 2026),
  and, to a limited extent, the shapes of broad emission lines (V. Rusakov et al.
  2026). While these features are consistent with the presence of dense, partially
  ionized gas, they stop short of providing direct spectroscopic confirmation of the
  physical conditions expected by the BH* scenario. What has been missing is an unambiguous
  demonstration—through emission-line physics—that LRDs indeed host dense, optically
  thick cocoons surrounding rapidly accreting black holes. Such evidence would directly
  tie the observed line formation, excitation, and radiative transfer to dense, stratified
  envelopes of gas surrounding the central engine.\r\n\r\nIn this work, we present
  precisely such a case: an exceptionally deep, ∼20 hr (equivalent to 80 hr without
  lensing magnification) JWST/NIRSpec G395M spectrum of a luminous LRD at z = 3.50102.
  The target, GLIMPSE-17775, lies in a highly magnified region of the massive galaxy
  cluster Abell S1063 (hereafter AS1063) and benefits from the combined power of JWST/NIRCam
  imaging from the GLIMPSE GO program (PID 3293; PIs: H. Atek & J. Chisholm) and recent
  NIRSpec spectroscopy from the GLIMPSEDirector's Discretionary Time (DDT) (hereafter
  GLIMPSE-D) program (PID 9223; PIs: S. Fujimoto & R. Naidu). This synergy of ultradeep
  spectroscopy and strong gravitational lensing enables an unprecedented view of GLIMPSE-17775,
  revealing rest-frame optical and NIR features at a level unseen before in any LRD.
  We detect over 40 emission and absorption features, including 16 Fe ii transitions
  that form a dense “iron forest.” The remarkable richness of this spectrum makes
  GLIMPSE-17775 a uniquely powerful laboratory for dissecting the dense, radiation-dominated
  environments that accompany early black hole growth.\r\n\r\nThis paper is organized
  as follows. In Section 2, we present the GLIMPSE-D NIRSpec dataset alongside the
  photometric datasets used in this study. In Section 3, we calculate the spectroscopic
  redshift, describe the identification of prominent emission/absorption features,
  and describe bespoke fitting of various line complexes. Section 4 describes the
  measurement of the source morphology, dust attenuation, and black hole masses. In
  Section 5, we comment on the various properties of the emission features in the
  our target. Finally, we discuss our findings in Section 6.\r\n\r\nThroughout this
  work, we assume a flat ΛCDM cosmology with Ωm,0 = 0.3, ΩΛ,0 = 0.7, and H0 = 70 km
  s−1 Mpc−1, and a G. Chabrier (2003) initial mass function between 0.1 and 100M⊙.
  All magnitudes are expressed in the AB system (J. B. Oke 1974).\r\n\r\n2. Observations
  and Data\r\nThe target, GLIMPSE-17775, was originally identified as a bright LRD
  candidate in JWST/NIRCam imaging captured by the GLIMPSE (PID: 3293; PIs: H. Atek
  & J. Chisholm) survey (H. Atek et al. 2025) of the lensed AS1063 Hubble Frontier
  Field (HFF; J. M. Lotz et al. 2017). The highly magnified area of AS1063 has already
  successfully yielded z  >  16 galaxy candidates (V. Kokorev et al. 2025), potential
  Population III (Pop III) hosts (S. Fujimoto et al. 2025a), numerous faint and high-redshift
  galaxies (I. Chemerynska et al. 2026), new constraints on reionization (D. Korber
  et al. 2025), identification of intermediate-mass black holes (Q. Fei et al. 2025),
  and a wide variety of enigmatic LRDs, some moderately lensed. The LRD selection
  was based on the standard compactness plus “V-shape” criteria already laid out in
  J. E. Greene et al. (2024), V. Kokorev et al. (2024a), H. B. Akins et al. (2025a),
  and I. Labbé et al. (2025) using photometric redshifts derived with eazy (G. B.
  Brammer et al. 2008), a technique that has proven successful at consistently identifying
  many exciting sources (see, e.g., H. B. Akins et al. 2025b; A. de Graaff et al.
  2025b; V. Kokorev et al. 2023; R. P. Naidu et al. 2025; A. J. Taylor et al. 2025).
  Located at zphot = 4.2 ± 0.1, GLIMPSE-17775 stood out in particular due to its extreme
  rest-optical brightness with mf444w ∼ 23.6 mag and a modest lensing magnification
  μ ∼ 2. While very little could be done with photometry alone, this marked GLIMPSE-17775
  as a promising target for any future spectroscopic follow-up.\r\n\r\n2.1. Photometry\r\nWe
  use photometry both to select targets for the GLIMPSE-D NIRSpec observations and,
  during spectroscopic modeling, to constrain the overall shape of the SED and correct
  for NIRSpec slit losses. In addition to JWST/NIRCam data, we incorporate deep HST
  Advanced Camera for Surveys and Wide Field Camera 3 imaging from the HFF (J. M.
  Lotz et al. 2017) and BUFFALO (C. L. Steinhardt et al. 2020) programs. Our reprocessed
  HST mosaics are based on Gaia-aligned images from the CHArGE archive (V. Kokorev
  et al. 2022), hosted on the Dawn JWST Archive (F. Valentino et al. 2023). More descriptions
  of the image reduction and source extraction procedure can be found in R. Endsley
  et al. (2025), as well as in the GLIMPSE overview paper (H. Atek et al. 2025); we
  briefly summarize the latter procedure below.\r\n\r\nPhotometry is performed on
  point-spread function (PSF)-homogenized HST and JWST images, convolved to the resolution
  of the F480M filter. Source detection is carried out using SExtractor (E. Bertin
  & S. Arnouts 1996) through two parallel steps. We construct two inverse-variance-weighted
  detection images: one from the short-wavelength (SW; F090W, F115W, F150W, F200W)
  bands to preserve spatial resolution, and one from the long-wavelength (LW; F277W,
  F356W, F444W) bands to ensure sensitivity to red or dusty sources (e.g., LRDs).
  Unlike the science images, these have not been PSF-matched. These SW and LW detection
  catalogs are subsequently merged into a single, combined catalog. Photometry is
  then measured using photutils (L. Bradley et al. 2020) in a range of circular apertures
  (–). Photometric uncertainties are estimated by placing random apertures in empty
  regions around each source. Unless stated otherwise, we adopt total fluxes measured
  within a aperture throughout this work.\r\n\r\n2.2. NIRSpec Observations\r\nGLIMPSE-D
  NIRSpec data were obtained during a campaign (DDT #9223; PIs: S. Fujimoto & R. Naidu)
  to study a promising Pop III galaxy candidate (S. Fujimoto et al. 2025a). GLIMPSE-D
  obtained a total of three G395M/F295LP MSA pointings, totaling 29.78 hr of total
  exposure time. The pointing center differed for each of the three configurations
  to maximize the total object yield. In total, the GLIMPSE-D sample contains 384
  spectra, with depths varying from 9.2 hr to ∼30 hr. All of the planned observations
  were successfully executed between 2025 June 30 and July 2. For each MSA configuration,
  GLIMPSE-D employed a standard three-point nod pattern at an aperture position angle
  PA_V3 = 2705, using 494 groups per integration with the NRSIRS2 readout mode. The
  full details of the target selection, prioritization, and MSA planning will be presented
  in a forthcoming survey paper (S. Fujimoto et al. 2025b).\r\n\r\n2.3. G395M Data
  Reduction and Calibration\r\nThe GLIMPSE-D MSA spectra were uniformly reduced using
  msaexp (v0.9.8; G. Brammer 2022). This procedure starts with the level-2 calibrated
  products obtained from MAST and applies a number of corrections that include 1/f
  noise, artifact detection and removal, and a bias correction in individual exposures
  (see J. Rigby et al. 2023 for more details). Together with the JWST pipeline, msaexp
  sets the slit World Coordinate System, performs flat-fielding, and computes an initial
  pass-loss correction. Each one of the two-dimensional shutters is then drizzled
  onto a common pixel grid. Using the standard approach, the background subtraction
  is performed locally using stacked, source-free shutters. The one-dimensional spectra
  are then obtained via the optimal extraction method (e.g., P. Arrabal Haro et al.
  2023; A. de Graaff et al. 2024), in which the center and width of the extraction
  “aperture” vary depending on the best-fit Gaussian model (K. Horne 1986), similar
  to the methodology widely adopted by a variety of other works (e.g., B. Wang et
  al. 2023; J. E. Greene et al. 2024; V. Kokorev et al. 2024b).\r\n\r\nThe absolute
  flux calibration of MSA spectra can be influenced by several factors, including
  the position of the source within the shutter, calibration and astrometric uncertainties,
  and the intrinsic morphology of the source. To correct for these effects and derive
  an overall slit-loss correction, we rescale the extracted one-dimensional spectra
  by convolving them with all available NIRCam filters and comparing the resulting
  flux densities to the total photometry from the GLIMPSE catalog. A wavelength-dependent
  correction is then obtained by fitting a second-order polynomial to these differences.\r\n\r\nThe
  target in this paper was observed in all three configurations; however, one was
  severely contaminated by sources in the same row, making the data recovery for that
  configuration unfeasible. Despite this, GLIMPSE-17775 is securely detected in two
  configurations (33,262 s and 40,703 s), yielding a total integration time of 20.55
  hr. We combine the extracted and separately calibrated one-dimensional spectra using
  inverse-variance weighting. The stacked spectrum is shown in Figure 1. We also make
  the spectrum publicly available.17\r\n\r\nZoom InZoom OutReset image size\r\nFigure
  1. Top: JWST/NIRCam and HST 20 stamps and red, green, blue short-wavelength (SW)
  and long-wavelength (LW) color images, comprising the F115W, F150W, and F200W and
  F277W, F356W, and F444W bands, respectively. MSA shutters for both configurations
  covering GLIMPSE-17775 are shown in blue and red, respectively. The source morphology
  is resolved and extended up to ∼2 μm, and then appears to transition to a more PSF-dominated
  and compact shape, echoing a growing sample of LRDs with extended rest-UV morphology
  (I. Juodžbalis et al. 2024; I. Labbe et al. 2024; J. Matthee et al. 2024; P. Rinaldi
  et al. 2025a). This likely hints at the presence of the host galaxy in the filters
  covering the rest-UV. In each panel, we show the total AB magnitude as presented
  in the GLIMPSE catalog (H. Atek et al. 2025; V. Kokorev et al. 2025). The source
  is exceptionally bright (M444 ∼ 23.6) and is detected in most JWST bands at >100σ.
  Middle: two-dimensional MSA G395M spectra covering GLIMPSE-17775. Bottom: combined
  one-dimensional spectrum (see, e.g., V. Kokorev et al. 2023; A. de Graaff et al.
  2025a for the extraction method) of the LRD in the observed frame. We show the data
  in black, and the uncertainty as a black shaded region. Fixing the systemic redshift
  to the [S iii] λ9071 line (zspec = 3.50102 ± 0.00019), we show the positions and
  label the prominent emission with significant (≥3σ) detections as solid vertical
  lines. Iron lines are shown separately in green. Due to the sheer number of features,
  not all could be labeled; we therefore display all features in Figure 2. Emission
  lines for which only upper limits are obtained are shown with dashed lines.\r\n\r\nDownload
  figure:\r\n\r\nStandard imageHigh-resolution image\r\n3. Emission-line Analysis\r\n3.1.
  Spectroscopic Redshift\r\nThe spectrum of GLIMPSE-17775 reveals a remarkably wide
  variety of significantly detected emission and absorption lines. Before focusing
  on individual features and their complex components, we perform an initial tally
  of all detectable lines using a heavily modified version of msaexp (G. Brammer 2022;
  V. Kokorev et al. 2024b). The key modifications allow varying the line widths and
  fitting multiple components, albeit tied to the same redshift.\r\n\r\nWe fit the
  full spectrum using msaexp, adopting Gaussian profiles for emission lines and a
  three-segment cubic spline to model the continuum. This minimal spline structure,
  appropriate given the high average S/N of GLIMPSE-17775 (≳30), helps prevent overfitting,
  particularly of features that may be slightly offset in wavelength or velocity space
  from the average redshift. Emission-line positions are fixed; narrow components
  are allowed a FWHM between 150 and 800 km s−1, and permitted transitions may include
  a broad component (800–5000 km s−1).\r\n\r\nThis yields a redshift of zspec = 3.5010
  ± 0.0001 (see Table 1). However, several strong lines exhibit significant pixel-level
  offsets of 100–200 km s−1 relative to this value. These discrepancies are statistically
  robust and appear in both stacked and individual spectra, suggesting that the derived
  redshift reflects a weighted average dominated by high-S/N lines. To properly assess
  velocity structure, a consistent systemic redshift is required. In the following
  sections describing the detailed line analysis, we adopt the centroid of a narrow
  forbidden line as the systemic reference frame (specifically [S iii] λ9071; see
  Section 3.3).\r\n\r\nUsing the updated redshift alongside the strong-lensing model
  of AS1063 (A. Zitrin et al. 2015; L. Furtak et al. 2026, in preparation), we recalculate
  the lensing magnification to be μ = 2.04 ± 0.21, consistent with previous estimates
  based on zphot. With redshift and magnification now fixed, we turn to a deeper analysis
  of the emission-line properties.\r\n\r\n3.2. Line Identification\r\nBeyond velocity
  offsets, the initial msaexp fit highlights several notable features. Broad hydrogen
  lines, ubiquitous in LRDs (e.g., D. D. Kocevski et al. 2023; V. Kokorev et al. 2023;
  L. J. Furtak et al. 2024; J. Matthee et al. 2024; A. de Graaff et al. 2025b; R.
  E. Hviding et al. 2025; R. P. Naidu et al. 2025; A. J. Taylor et al. 2025), are
  strongly favored across the Balmer and Paschen series, with Δχ2 > 10. These include
  Hα and Pa10 through Paγ. Although Paβ falls near the edge of the detector, we nonetheless
  observe a prominent broad wing at its expected location (see Figure 1).\r\n\r\nBroad
  components are also detected in several helium and oxygen lines: He i λ6680, He
  i λ7065, O i λ8448, He i λ10830, and O i λ11290. Notably, the He i λ10830 line shows
  a classic P-Cygni profile with a clear blueshifted absorption trough. While Balmer
  absorption is becoming a familiar sight in LRDs (R. Maiolino et al. 2024; J. Matthee
  et al. 2024; A. de Graaff et al. 2025b; D. D. Kocevski et al. 2025; R. P. Naidu
  et al. 2025), helium absorption remains rare, with only a few published cases at
  high z (e.g., I. Juodžbalis et al. 2024; R. P. Naidu et al. 2024; B. Wang et al.
  2025). Curiously, this was also recently reported in local analogs of LRDs (X. Lin
  et al. 2026).\r\n\r\nThe most striking feature is the detection of an extensive
  Fe ii emission forest in the rest-NIR—at least 16 distinct features are identified
  by msaexp and highlighted in green in Figure 1. Previous detections of permitted
  Fe ii in LRDs have been mostly limited to rest-UV/optical wavelengths using low-resolution
  PRISM spectra (R. Tripodi et al. 2025), with only few examples in the NIR (e.g.,
  see broad Fe iiλ9200 I. Labbe et al. 2024). Iron has also been identified in local
  LRD analogs (X. Lin et al. 2026; X. Ji et al. 2026). Only recently have a few Fe
  ii emitters been reported in medium-resolution (F. D’Eugenio et al. 2025) and high-resolution
  spectra (A. Torralba et al. 2026). The richness of these lines in GLIMPSE-17775
  hints at a dense, partially shielded gas phase, where processes such as Lyβ fluorescence
  and continuum pumping may be enhancing Fe ii emission (T. A. A. Sigut & A. K. Pradhan
  1998, 2003; T. A. A. Sigut et al. 2004), offering a new diagnostic window into early
  AGN environments.\r\n\r\nIn summary, GLIMPSE-17775 exhibits an exceptionally rich
  and kinematically complex array of emission and absorption features. While the initial
  msaexp modeling provides a solid foundation for redshift estimation and line identification,
  it lacks the flexibility to capture the full diversity of line profiles in this
  high-S/N dataset. In the following sections, we peel back the spectral layers with
  increasing precision.\r\n\r\n3.3. Line Fitting\r\nThe exceptional depth of the G395M
  spectrum for GLIMPSE-17775 enables detailed modeling of both multiple kinematic
  components and potential velocity offsets between line species. Unless noted otherwise,
  each line is fit with a single Gaussian narrow component (FWHM = 100−800 km s−1).
  For permitted lines flagged by msaexp as potentially broad, we follow the approach
  of V. Rusakov et al. (2026) and model the profile as an intrinsic Gaussian core
  broadened by electron scattering, implemented via convolution with an exponential-wing
  component. The intrinsic Gaussian FWHM is allowed to vary between 500 and 5000 km
  s−1. The characteristic scattering width (i.e., the strength of the exponential
  wings, W) is treated as a free parameter and is allowed to vary independently between
  different transitions. For each broad line, we also perform an alternative fit with
  the W parameter fixed to zero (pure Gaussian) and compare the resulting goodness
  of fit to assess whether the exponential wings are statistically required. Line
  centers are allowed to vary independently unless otherwise specified.\r\n\r\nAbsorption
  lines are modeled using a Gaussian optical-depth profile, where the observed flux
  is Fobs = Fem e−τ(λ), where . The free parameters are then the central optical depth
  τ0, velocity width Δvabs, and redshift zabs (see I. Juodžbalis et al. 2024). Widths
  and redshifts (for both narrow and broad components) are typically free, with redshift
  limited to ± 0.1 from the msaexp value. Local continua are fit using first-order
  polynomials.\r\n\r\nAll individual model components are first initialized and coadded
  on an oversampled wavelength grid. To take into account the wavelength-dependent
  resolution of the grating, we interpolate our model onto a variable step grid while
  making sure that the total integrated flux is preserved. Further, we increase the
  nominal spectral resolution by a factor of 1.7, as it has been shown that the spectral
  resolution for a pointlike source falling within a shutter is higher than that of
  a uniformly illuminated slitlet (A. de Graaff et al. 2024). Fitting uses nonlinear
  χ2 minimization, with uncertainties derived from multivariate resampling of the
  covariance matrix.\r\n\r\nTable 1. Source Properties\r\n\r\nParametera\tGLIMPSE-17775\r\nID\t17775\r\nR.A.
  [deg]\t342.20080\r\nDecl. [deg]\t–44.54366\r\nzphot (eazy)\t4.2 ± 0.1\r\nzspec ([S
  iii] λ9071)\t3.50102 ± 0.00019\r\nμ\t2.04 ± 0.21\r\nMUV [AB mag]\t−17.27 ± 0.05\r\nreff,UV
  [pc]\t1000 ± 200\r\nreff,opt [pc]\t<300\r\nβ\t–0.69 ± 0.12\r\nlog10(MBH/M⊙)\t6.65
  ± 0.15\r\nLbol [erg s−1]\t(1.06 ± 0.14)×1045\r\nλedd\t1.86 ± 0.25\r\nlog10(M*/M⊙)\t<7.5\r\nAV\t0.1
  ± 0.3\r\nfν,4050Å/fν,3670Å\t2.02 ± 0.10\r\nNote. aPhysical parameters are corrected
  for the lensing magnification.\r\n\r\nDownload table as: \r\nASCIITypeset image\r\n\r\nGiven
  the complexity, the spectrum is divided into six windows grouped by line species
  or proximity (see Figure 2). Below, we describe the assumptions adopted for each
  window. Final fluxes and equivalent widths of the narrow and broad lines are listed
  in Tables 2 and 3, respectively, while kinematics are reported in Tables 4 and 5.
  We show detailed line fits in Figure 2.\r\n\r\nZoom InZoom OutReset image size\r\nFigure
  2. A staggering abundance of spectral lines in GLIMPSE-17775 at z = 3.501. For each
  spectral window defined in Section 3.3, we show the data (black), the best-fit narrow
  and broad components (dark purple and blue), and the total best-fit model including
  the continuum (red). All broad components were fit with models allowing exponential
  wings. The ΔBIC between exponential and Gaussian fits is reported in the top right
  of each panel; negative values indicate a preference for an exponential profile.
  The lower panels display the uncertainty-weighted residuals for each fit.\r\n\r\nDownload
  figure:\r\n\r\nStandard imageHigh-resolution image\r\nTable 2. Fluxes of Narrow
  Emission Lines and Their Rest-frame Equivalent Widthsa\r\n\r\nLine\tλrest\tFlux\tEW0\r\n
  \t(Å)\t(10−20 erg s−1 cm−2)\t(Å)\r\nNarrow Emission Lines\r\nO i\t6302.0\t54.0 ±
  21.2\t3.3 ± 1.2\r\n[N ii]\t6549.0\t25.6 ± 10.3\t1.6 ± 0.7\r\nHα\t6562.8\t2622.9
  ± 200.7\t167.7 ± 12.8\r\n[N ii]\t6584.0\t77.1 ± 37.1\t4.9 ± 1.6\r\nHe i\t6680.0\t14.7
  ± 11.1\t0.8 ± 0.7\r\n[S ii]\t6717.0\t22.2 ± 0.1\t1.5 ± 0.7\r\n[S ii]\t6731.0\t21.4
  ± 0.1\t1.4 ± 0.5\r\nHe i\t7065.0\t461.7 ± 210.2\t31.0 ± 12.2\r\n[Ar iii]\t7138.0\t12.6
  ± 3.4\t1.0 ± 0.3\r\nFe ii\t7156.0\t26.2 ± 7.2\t1.8 ± 0.2\r\n[O ii]\t7323.0\t26.0
  ± 23.0\t1.7 ± 1.5\r\n[O ii]\t7325.0\t16.9 ± 1.8\t1.2 ± 0.1\r\n[O ii]\t7332.0\t26.2
  ± 9.1\t1.8 ± 0.6\r\nFe ii\t8228.0\t23.7 ± 4.2\t2.0 ± 0.3\r\nFe ii\t8239.0\t7.2 ±
  4.0\t0.6 ± 0.3\r\nFe ii\t8289.0\t6.3 ± 3.7\t0.5 ± 0.3\r\nFe iii\t8306.0\t5.7 ± 3.6\t0.5
  ± 0.3\r\nO i\t8448.0\t67.6 ± 2.4\t6.1 ± 1.3\r\nFe ii\t8470.0\t16.2 ± 5.0\t1.4 ±
  0.4\r\nFe ii\t8490.0\t26.7 ± 4.3\t2.4 ± 0.4\r\nPa10\t9015.0\t16.5 ± 5.0\t1.8 ± 0.5\r\n[S
  iii]\t9071.0\t27.2 ± 2.3\t3.5 ± 0.3\r\nFe ii\t9075.0\t30.0 ± 4.7\t3.4 ± 0.5\r\nFe
  ii\t9125.0\t16.8 ± 5.2\t1.9 ± 0.6\r\nFe ii\t9134.0\t36.9 ± 5.0\t4.1 ± 0.6\r\nFe
  ii\t9179.0\t95.0 ± 5.5\t10.6 ± 0.6\r\nFe ii\t9204.0\t50.1 ± 6.1\t5.6 ± 0.7\r\nPa9\t9229.0\t19.4
  ± 7.0\t2.2 ± 0.8\r\nFe ii\t9394.0\t17.3 ± 3.9\t2.0 ± 0.5\r\n[S iii]\t9533.0\t84.7
  ± 5.9\t10.2 ± 0.7\r\nPa8\t9545.0\t44.8 ± 11.3\t5.4 ± 1.4\r\nFe ii\t9997.0\t29.5
  ± 4.5\t3.8 ± 0.6\r\nPaδ\t10049.0\t104.2 ± 12.2\t13.7 ± 1.7\r\nFe ii\t10490.0\t8.0
  ± 2.7\t1.1 ± 0.4\r\nFe ii\t10501.0\t24.4 ± 5.9\t3.1 ± 0.8\r\nHe i\t10830.0\t163.0
  ± 96.0\t22.6 ± 13.3\r\nPaγ\t10938.0\t146.3 ± 25.5\t20.9 ± 3.8\r\nFe ii\t11128.0\t12.3
  ± 3.7\t1.8 ± 0.6\r\nO i\t11290.0\t49.2 ± 4.1\t7.7 ± 2.3\r\nNote. aNot corrected
  for lensing magnification.\r\n\r\nDownload table as: \r\nASCIITypeset image\r\n\r\nTable
  3. Fluxes of Broad Emission Lines and Their Rest-frame Equivalent Widthsa\r\n\r\nLine\tλrest\tFlux\tEW0\r\n
  \t(Å)\t(10−20 erg s−1 cm−2)\t(Å)\r\nBroad Emission Lines\r\nHα\t6562.8\t14803.5
  ± 198.6\t946.3 ± 15.6\r\nHe i\t6680.0\t144.6 ± 44.7\t9.4 ± 2.9\r\nHe i\t7065.0\t824.2
  ± 210.0\t55.4 ± 15.1\r\nPa10\t9015.0\t53.7 ± 11.1\t5.8 ± 1.3\r\nPa9\t9229.0\t119.0
  ± 13.5\t13.6 ± 1.5\r\nPa8\t9545.0\t191.2 ± 17.0\t23.1 ± 2.1\r\nPaδ\t10049.0\t370.6
  ± 15.0\t48.8 ± 2.3\r\nHe i\t10830.0\t2294.9 ± 212.6\t318.8 ± 30.3\r\nPaγ\t10938.0\t652.3
  ± 14.0\t92.9 ± 2.4\r\nO i\t8448.0\t93.7 ± 7.9\t8.4 ± 0.7\r\nO i\t11290.0\t106.2
  ± 63.9\t16.6 ± 10.4\r\nNote. aNot corrected for lensing magnification.\r\n\r\nDownload
  table as: \r\nASCIITypeset image\r\n\r\nTable 4. Kinematic Properties of Narrow
  Lines\r\n\r\nLine\tλrest\tFWHM\tΔv\r\n \t(Å)\t(km s−1)\t(km s−1)\r\nNarrow Emission
  Lines\r\n[O i]\t6300.3\t455 ± 175\t−101 ± 81\r\nHα\t6562.8\t304 ± 8\t+145 ± 13\r\n[N
  ii]\t6583.4\t347 ± 117\t+84 ± 47\r\n[S ii]\t6716.4\t232 ± 62\t+82 ± 33\r\n[S ii]\t6731\t232
  ± 62\t+82 ± 33\r\nHe i\t6678.2\t87 ± 14\t+40 ± 14\r\nHe i\t7065.2\t408 ± 644\t+112
  ± 396\r\n[Ar iii]\t7135.8\t89 ± 50\t−26 ± 20\r\nFe ii\t7155.2\t96 ± 50\t+15 ± 15\r\n[O
  ii]\t7320.0\t400 ± 120\t−37 ± 72\r\nFe ii\t8228.0\t290 ± 48\t+21 ± 5\r\nFe ii\t8239.0\t290
  ± 48\t+21 ± 5\r\nFe ii\t8289.0\t290 ± 48\t+21 ± 5\r\nFe iii\t8306.0\t290 ± 48\t+21
  ± 5\r\nO i\t8446.4\t235 ± 30\t−43 ± 19\r\nFe ii\t8470.0\t290 ± 48\t+21 ± 5\r\nFe
  ii\t8490.0\t290 ± 48\t+21 ± 5\r\nPa10\t9014.9\t259 ± 36\t−46 ± 19\r\n[S iii]\t9071.0\t230
  ± 13\t⋯\r\nFe ii\t9075.0\t486 ± 24\t−21 ± 17\r\nFe ii\t9125.0\t486 ± 24\t−21 ± 17\r\nFe
  ii\t9134.0\t486 ± 24\t−21 ± 17\r\nFe ii\t9179.0\t486 ± 24\t−21 ± 17\r\nFe ii\t9204.0\t486
  ± 24\t−21 ± 17\r\nPa9\t9229.0\t259 ± 35\t−46 ± 19\r\nFe ii\t9394.0\t486 ± 24\t−21
  ± 17\r\nPa8\t9545.6\t259 ± 36\t−46 ± 19\r\n[S iii]\t9533\t230 ± 13\t+23 ± 13\r\nFe
  ii\t9997.0\t331 ± 55\t+90 ± 25\r\nPaδ\t10049.4\t332 ± 22\t+21 ± 15\r\nHe i\t10830.3\t287
  ± 46\t+112 ± 26\r\nPaγ\t10938.1\t267 ± 25\t+26 ± 17\r\nFe ii\t10490.0\t332 ± 96\t+44
  ± 43\r\nFe ii\t10501.0\t332 ± 96\t+44 ± 43\r\nFe ii\t11128.0\t153 ± 116\t+37 ± 30\r\nO
  i\t11290.0\t260 ± 58\t−33 ± 24\r\nNote. Velocity offsets (Δv) calculated relative
  to [S iii] λ9071 at z = 3.50102.\r\n\r\nDownload table as: \r\nASCIITypeset image\r\n\r\nTable
  5. Kinematic Properties of Broad and Absorption Lines\r\n\r\nLine\tλrest\tFWHM\tW\tΔv\r\n
  \t(Å)\t(km s−1)\t(km s−1)\t(km s−1)\r\nBroad Emission Lines\r\nHα\t6562.8\t1024
  ± 21\t3010 ± 450\t−7 ± 16\r\nHe i\t6678.2\t1041 ± 792\t3890 ± 2083\t−137 ± 151\r\nHe
  i\t7065.2\t473 ± 116\t1000 ± 600\t−136 ± 82\r\nO i\t8446.4\t562 ± 331\t1120 ± 590\t+39
  ± 80\r\nPa10\t9014.9\t766 ± 202\t2100 ± 600\t−155 ± 39\r\nPa9\t9229.0\t766 ± 202\t2100
  ± 600\t−155 ± 39\r\nPa8\t9545.6\t766 ± 202\t2100 ± 600\t−155 ± 39\r\nPaδ\t10049.4\t1672
  ± 458\t3500 ± 400\t+23 ± 44\r\nHe i\t10830.3\t536 ± 45\t2760 ± 220\t+154 ± 22\r\nPaγ\t10938.1\t1035
  ± 322\t2400 ± 260\t−75 ± 31\r\nO i\t11287.0\t1188 ± 1099\t4300 ± 2000\t+245 ± 214\r\nAbsorption
  Lines\r\nHα\t6562.8\t1000 ± 123\t⋯\t−200 ± 32\r\nHe i\t7065.2\t587 ± 1024\t⋯\t−52
  ± 83\r\nHe i\t10830.3\t794 ± 21\t⋯\t+45 ± 22\r\nNote. Velocity offsets (Δv) calculated
  relative to [S iii] λ9071 at z = 3.50102.\r\n\r\nDownload table as: \r\nASCIITypeset
  image\r\n\r\n3.3.1. Hα Complex\r\nHα is modeled with independent narrow, broad,
  and absorption components. [O i] λ6302 and He i λ6680 are modeled with narrow and
  broad profiles. [N ii] lines are fixed at a 1:3 ratio and share kinematics; [S ii]
  lines have independent amplitudes but tied velocities and widths.\r\n\r\nWe find
  that broad Hα and He i λ6680 are strongly favored to have exponential wings (ΔBIC
  ∼ −500), yielding a FWHM (of the intrinsic Gaussian core) of ∼1000 km s−1—significantly
  narrower than the ∼3000 km s−1 derived from pure Gaussians. Although no distinct
  Hα absorption component is explicitly detected, likely due to insufficient resolution,
  the overall asymmetry of the line is best reproduced when a weak, blueshifted absorber
  is included in the fit. This may indicate subtle self-absorption or partial obscuration
  within the dense cocoon. We return to the implications of this profile shape later.\r\n\r\n3.3.2.
  He i λ7065\r\nThe He i λ7065 line shows a prominent blueshifted absorption component.
  We fit it with narrow, broad, and absorption profiles. The rest of the lines, including
  [Ar iii] λ7138, Fe ii λ7156, and the [O ii] triplet (λλ7323, 7325, 7332), are modeled
  as independent narrow lines.\r\n\r\nHe i λ7065 shows a strong preference for an
  exponential profile (ΔBIC ∼ − 16) with a FWHM = 473 ± 116 km s−1. A residual bump
  spanning from ∼λ7290 to λ7320 is likely a combination of multiple Fe ii, such as
  λ7290, λ7308, and potentially Fe iii λ7319.65 lines. Curiously, the latter line
  is often labeled as “hazy” in various emission-line libraries (e.g., A. Kramida
  et al. 2024), reflecting its undefined shape as a result of pressure broadening
  or scattering in very dense gas.\r\n\r\n3.3.3. O i λ8448 and Iron Lines\r\nIn this
  part of the spectrum the O i λ8448 is fit with narrow and broad components. All
  of the iron lines, including Fe ii λλ8228, 8239, 8289, 8470, 8490 as well as a potential
  Fe iii λ8306, are fit as narrow lines with shared kinematics. O i components are
  fit independently.\r\n\r\nWe find that the broad O i component is best described
  by a standard Gaussian profile, with a stronger statistical preference over exponential
  wings (ΔBIC ∼ 4). However, we caution that a trough at ∼3.77 μm, likely an artifact,
  may affect the reliability of the fit in this region.\r\n\r\n3.3.4. Iron Forest
  and Paschen Lines\r\nThis spectral region is among the most complex, due to the
  dense clustering of emission features. The Paschen lines Pa10–Pa8 are modeled with
  narrow and broad components. To reduce the number of free parameters, we tie all
  narrow Paschen components together kinematically, and do the same for the broad
  components. Fe ii λλ9075, 9125, 9134,9179, 9204, 9394 are fit with a shared centroid
  and width. [S iii] lines are fit independently.\r\n\r\nThe [S iii] λ9071 line is
  used to define the systemic redshift: z = 3.50102 ± 0.00019. This is done because
  forbidden lines, such as [S iii] or [O iii], have lower critical densities that
  are incompatible with the dense-gas envelopes giving rise to the other lines we
  observe. These lines may instead come from the host galaxy itself (e.g., R. Maiolino
  et al. 2024), and we therefore choose this line to define the overall redshift of
  the system and to measure all the offsets relative to it. All velocity offsets discussed
  in the subsequent sections are computed relative to this reference frame. The Paschen
  lines show strong preference for exponential wings (ΔBIC ∼ −38), with a FWHM = 766
  ± 202 km s−1—narrower than Hα, but consistent within 2σ.\r\n\r\n3.3.5. Paδ\r\nThe
  Fe ii λ9997 and Paδ complex is modeled with an independent narrow component for
  Fe ii and both narrow and broad components for Paδ. There is no evidence for absorption.
  Exponential wings are again preferred (ΔBIC ∼ −26). The resulting FWHM of 1672 ±
  458 km s−1 is notably larger than those of both higher-order Paschen lines and Hα,
  though still consistent with the latter within 2σ. It is also possible that the
  line shape is impacted by Fe ii λ9997 and the undetected (but likely present) Fe
  ii λλ10131, 10173 lines.\r\n\r\n3.3.6. He i λ10830 and Paγ\r\nThe final window contains
  a complicated blend of broad He i λ10830 and Paγ lines, with a clear blueshifted
  absorption in the former. We fit three components (narrow, broad, and absorption)
  to He iλ10830 and narrow plus broad components to Paγ, keeping everything kinematically
  independent. We fit narrow Fe ii lines at 10490, 10501, and 11128 Å with fixed redshift
  and line width. Finally, O i λ11290 is fit with independent narrow and broad components.
  Exponential wings are again preferred over a pure Gaussian profile.\r\n\r\n4. Data
  Analysis\r\n4.1. Morphology\r\nLRDs are unresolved in the rest-optical by definition,
  with measured sizes consistent with the PSF HWHM ( in F444W), and in some cases
  even smaller when dithers align favorably (e.g., I. Labbé et al. 2025). Gravitational
  lensing can further push constraints on their intrinsic sizes to ≲100 pc (L. J.
  Furtak et al. 2024).\r\n\r\nIn the rest-UV, however, a more complex picture is emerging.
  Several studies have now reported faint, extended, asymmetric components adjacent
  to the compact core (V. Kokorev et al. 2024b; I. Labbe et al. 2024; J. Matthee et
  al. 2024; P. Rinaldi et al. 2025a, 2025b), often suppressed by surface-brightness
  dimming. As shown in Figure 1, GLIMPSE-17775 likewise consists of two components
  out to F200W (rest ∼ 4000 Å), coincident with the Balmer break. However, we note
  that the break itself is much weaker than found in objects with very similar spectra
  (e.g., B. Wang et al. 2024; see Figure 3). At longer wavelengths, a point-source
  (PS) morphology dominates, consistent with a black-hole-dominated core. To quantify
  this transition, we model the NIRCam imaging using PYSERSIC (I. Pasha & T. B. Miller2023)
  with a minimal configuration: a fixed-center PS plus a freely offset Sérsic profile.
  Normalizations, n, and reff are all allowed to vary, and uncertainties are drawn
  from the Markov Chain Monte Carlo posteriors (e.g., V. Kokorev et al. 2024a).\r\n\r\nZoom
  InZoom OutReset image size\r\nFigure 3. The diversity of Balmer breaks in LRDs.
  The black points show the HST and JWST GLIMPSE photometry of GLIMPSE-17775. The
  blue line shows best-fit EAZY SED fit to the photometry only, fixing the redshift
  to the zspec. The maroon line show the combined and photometry-corrected G395M spectrum.
  While the red color in F200W–F277W is partially influenced by a bright Hα line,
  the Balmer break between F150W and F200W is still prominent. We further show spectra
  of various other LRDs (I. Labbe et al. 2024; B. Wang et al. 2024; A. de Graaff et
  al. 2025b; R. P. Naidu et al. 2025; A. J. Taylor et al. 2025), all shifted to z
  = 3.501 and normalized at 5100 Å. Finally, we show HST (blue) and JWST (orange)
  filter transmission curves below.\r\n\r\nDownload figure:\r\n\r\nStandard imageHigh-resolution
  image\r\nOur fits show that the host galaxy dominates up to λrest ∼ 4000 Å, where
  the host and nucleus contribute roughly equally, beyond which the PS prevails to
  λrest ∼ 1 μm. Because the NIRCam LW detector has ≳2× poorer resolution than the
  SW, a clean separation of host and nucleus in the rest-optical is impractical (see,
  e.g., K. E. Whalen et al. 2026). Fortunately, F200W lies at the transition where
  both the resolution and flux ratio are favorable, so we use that band to illustrate
  our galaxy/LRD decomposition. We illustrate this in Figure 4, which also shows the
  increasing PS fraction with wavelength, while acknowledging the uncertainties at
  longer wavelengths.\r\n\r\nZoom InZoom OutReset image size\r\nFigure 4. Top: two-component
  Sérsic+point-source (PS) fit to the F200W morphology of GLIMPSE-17775. Panels show,
  from left to right, the data, best-fit model, model with the extended component
  removed, and residuals. Bottom: fractional PS contribution vs. rest-frame wavelength.
  Shaded regions mark SW (blue) and LW (red) detectors, where the lower resolution
  of LW filters hinders reliable two-component decomposition.\r\n\r\nDownload figure:\r\n\r\nStandard
  imageHigh-resolution image\r\nAfter applying the lensing correction, we find that
  the extended component dominating the UV light has a radius of reff ∼ 1000 pc, whereas
  the actual compact LRD, dominant in the rest-optical, is fully consistent with the
  PSF and reff < 300 pc.\r\n\r\n4.2. Dust Attenuation\r\nThe ratio between observed
  emission-line fluxes is commonly used to estimate dust extinction. For LRDs, this
  has typically been achieved through the Balmer decrement, provided that multiple
  Balmer lines are available. In our case, only Hα is detected. While the Paschen
  series, of which five lines are observed, could, in principle, be used to estimate
  extinction, the likely presence of stratified dense gas in LRDs (A. de Graaff et
  al. 2025b; R. P. Naidu et al. 2025) implies that the intrinsic line ratios may deviate
  significantly from standard Case B recombination expectations (S.-J. Chang et al.
  2026). Further, at the wavelengths of the Paschen series, the attenuation curves
  are practically flat (e.g., D. Calzetti et al. 2000). Small offsets of the Case
  B ratios would have a significant effect on the derived dust attenuation, but in
  return require extreme precision on measured line fluxes to be meaningful. Our uncertainties
  on, e.g., Paγ/Paδ are small, roughly 10%–15%, yet this still leads to an impractically
  high uncertainty on AV. To circumvent this limitation, we instead employ the ratio
  between the permitted O i λ8448 and O i λ11290 lines.\r\n\r\nThese transitions share
  a common energy level, and under the assumption of Bowen (Lyβ) fluorescence, all
  transitions through the λ11290 transition also cascade through the λ8448. This makes
  their intrinsic intensity set solely by the ratio of the inverse of their wavelengths.\r\n\r\nTo
  ensure we are comparing the same physical gas component, we isolate the narrow emission
  peaks in both transitions, which show consistent widths of FWHM ∼ 250 km s−1. This
  similarity supports the use of their flux ratio as a dust probe. We adopt the Small
  Magellanic Cloud (SMC) attenuation curve (K. D. Gordon et al. 2003), widely used
  for high-redshift galaxies and reddened AGN (P. F. Hopkins et al. 2004; P. L. Capak
  et al. 2015; N. A. Reddy et al. 2015, 2018; V. Kokorev et al. 2023; A. J. Taylor
  et al. 2025). Assuming an intrinsic ratio of (8448/11290)int = 1.336 (D. E. Osterbrock1989),
  we infer AV = 0.1 ± 0.3 mag, consistent with negligible extinction.\r\n\r\nWe caution,
  however, that this ratio probes only the narrow-line-emitting gas, which could originate
  either in the host galaxy or within a narrow-line region associated with the AGN.
  If the latter is the case, then the red optical continuum slope (βopt ∼ 0.35) would
  suggest that the observed SED is intrinsically red rather than reddened by dust.
  If instead the narrow lines arise predominantly in the host galaxy, this constraint
  does not directly inform the origin of the continuum emission. Similar Case B–consistent
  narrow-line ratios have been reported in other LRDs (e.g., M. Brooks et al. 2025;
  G. P. Nikopoulos et al. 2025), where the broad lines were found to show significant
  departures from Case B.\r\n\r\nAlthough the wavelength coverage of the red grating
  does not allow a Balmer decrement test for the broad-line emission (only Hα is detected),
  we can perform a consistency check using the brightest broad Paschen lines (Paγ,
  Paδ, and Pa8). Adopting intrinsic Case B ratios from P. J. Storey & D. G. Hummer
  (1995; Paγ/Paδ ≃ 1.5 and Paδ/Pa8 ≃ 1.8), and comparing these to our measured values
  of Paγ/Paδ = 1.77 ± 0.15 and Paδ/Pa8 = 1.94 ± 0.20, we find the broad Paschen lines
  to be consistent with Case B within ≃2σ, particularly when systematic uncertainties
  from blending and profile decomposition are taken into account. If Case B is applicable
  in the dense environments surrounding the central AGN, this would be consistent
  with a low-dust or dust-free origin for the broad-line-emitting gas.\r\n\r\n5. Line
  Properties\r\nOur fitting procedure yields over 40 emission and absorption features,
  most of which are detected at a high (S/N> 3) significance. With all the pieces
  in place, we now comment on the line profiles, kinematics, and the specific line
  species that we identify.\r\n\r\n5.1. Exponential Wings\r\nAs already noted throughout
  Section 4, and further highlighted in Figure 2, all permitted lines in the spectrum,
  with the exception of O iλ8448, which is likely impacted by data-quality issues,
  are better fit when the broad component is convolved with an exponential profile.
  The statistical preference for this model (as measured by ΔBIC) is especially strong
  for our brightest line, Hα. To further demonstrate this, and to compare this fit
  with a more standard, Gaussian-only approach, we show both models in Figure 5. When
  the broad line is fit using only a Gaussian profile, large portions of the line
  are underfit at a ≳3σ significance level, whereas a model that includes exponential
  wings shows a much smoother, albeit not perfect, residual plot.\r\n\r\nZoom InZoom
  OutReset image size\r\nFigure 5. Exponential wings are required. Comparison of a
  Gaussian×exponential model (red) and a single Gaussian profile (blue) for Hα. Uncertainties
  are shown as vertical lines in each spectral bin, although they are too small to
  be visible. The exponential model provides a far superior fit, with smoother residuals
  and a strongly preferred ΔBIC, highlighting the necessity of exponential wings to
  capture the broad-line shape.\r\n\r\nDownload figure:\r\n\r\nStandard imageHigh-resolution
  image\r\nThis strong preference for exponential wings is consistent with expectations
  from electron scattering in dense, ionized gas. Unlike Gaussian profiles, which
  arise from Doppler broadening due to thermal and bulk motions around the supermassive
  black hole, exponential profiles arise in environments dominated by electron scattering
  (e.g., S.-J. Chang et al. 2026; V. Rusakov et al. 2026). The absence of strong broadening
  in the forbidden lines (e.g., [S ii], [S iii], and [N ii]) already suggests that
  the densities where these electron-scattered profiles originate must already exceed
  multiple times the critical densities of these transitions (ne > 106). Combined
  with the fact that these broad profiles are non-Gaussian in shape, both the likely
  volume and column densities are likely even higher, at ne = 108 cm−3 and Ne ∼ 1024
  cm−2, respectively, as suggested by both K. Inayoshi & R. Maiolino (2025) and V.
  Rusakov et al. (2026).\r\n\r\nRecent work (e.g., M. Brazzini et al. 2025) argues
  that, in classical broad-line region (BLR) environments, an electron-scattering
  origin for broad wings requires similar intrinsic and scattering widths across recombination
  lines. We therefore examine these criteria for the hydrogen transitions and find
  that, within the uncertainties of our fits, both the intrinsic and exponential widths
  are broadly comparable among the recombination lines. However, unlike classical
  BLRs, LRDs are expected to be strongly stratified, with different recombination
  transitions forming at different depths and probing different effective electron
  columns (e.g., A. de Graaff et al. 2025d; A. Sneppen et al. 2026). In such a structure,
  strict equality of widths is not expected even if a common scattering kernel shapes
  the wings. The modest variations observed here are therefore consistent with electron
  scattering in a dense, stratified cocoon.\r\n\r\nIt is important to note that such
  detailed profile decomposition is only possible due to the exceptionally high S/N
  per pixel achieved in the line wings of our NIRSpec G395M spectrum. As emphasized
  in V. Rusakov et al. (2026), these features would be impossible to distinguish with
  shallower data or lower-resolution modes such as NIRSpec/PRISM, or even G395M exposures
  lacking comparable depth.\r\n\r\n5.2. Line Profiles\r\nFurther, in Figure 6, we
  compare the best-fit models for all broad lines. As noted previously, with the exception
  of O i λ8448, every broad line is better described by exponential wings, resulting
  in very similar overall line shapes. The main differences arise in their widths.\r\n\r\nZoom
  InZoom OutReset image size\r\nFigure 6. Best-fit profiles of all broad lines, oversampled
  and shifted to a common center. The top panel shows hydrogen recombination (Hα,
  black, and Paschen series), the middle panel shows O i, and the bottom panel shows
  He i. Shaded regions indicate 1σ uncertainties for the least-constrained lines (Paδ,
  O i λ11290, and He i λ6680); uncertainties for the remaining lines are omitted for
  clarity. We note that hydrogen and O i lines show largely similar widths, consistent
  with their coupling through charge exchange. By contrast, He i lines are systematically
  narrower, likely reflecting their distinct metastable triplet physics and formation
  in a less dense outer region.\r\n\r\nDownload figure:\r\n\r\nStandard imageHigh-resolution
  image\r\nDespite some fits having sizable uncertainties, a trend emerges across
  line species. Hydrogen recombination lines (with the exception of Paδ) and O i transitions
  consistently show comparable intrinsic FWHM values of ∼800 km s−1. This agreement
  is not coincidental. Neutral oxygen and ionized hydrogen have nearly identical ionization
  potentials, enabling rapid charge-exchange coupling between O+ + H0⇌ O0 + H+ (D.
  E. Osterbrock & G. J. Ferland 2006). This continual electron exchange tightly locks
  the spatial distribution, ionization state, and kinematics of neutral oxygen to
  ionized hydrogen (and vice versa), so their broad-line profiles are naturally expected
  to track one another. The observed similarity therefore provides an important consistency
  check, reinforcing that the O i emission originates in the same dense, ionized gas
  as the hydrogen recombination lines. In contrast, the Fe ii lines exhibit significantly
  narrower widths, matching the narrow cores of the permitted transitions rather than
  their exponential wings. This implies that the Fe ii emission arises in a cooler,
  less turbulent zone exterior to the scattering-dominated region, but still closely
  coupled to the AGN continuum source.\r\n\r\nBy contrast, He i emission is systematically
  narrower. He i lines such as λ7065 and λ10830 do not couple to hydrogen via charge
  exchange, and their lower metastable level (23S) has distinct population physics,
  being fed by both collisional and recombination pathways. Further, one has to take
  into account the radiative-transfer effects, which make it possible to radiatively
  excite metastable ground-state electrons. As a result, He i emission may arise from
  a somewhat different spatial or kinematic region than H and O. We return to this
  point in more detail below.\r\n\r\nTaken together, the similar FWHM of hydrogen
  and oxygen broad-line profiles, combined with the near-universal exponential wings
  seen across all permitted transitions, strongly suggests that the line shapes are
  set by a common, line-independent scattering kernel rather than by transition-specific
  processes. Electron (Thomson) scattering in a dense, ionized cocoon provides a natural
  explanation: It produces exponential wings of nearly identical form across species,
  with widths set primarily by the electron temperature and column density (typically
  ∼1024 cm−2), and leaves only secondary variations from species-specific excitation
  or optical-depth effects (e.g., S.-J. Chang et al. 2026; V. Rusakov et al. 2026).
  In this framework, the narrower He i lines reflect stratification within the cocoon,
  where He i emission arises from an outer region that has a lower density, temperature,
  or column density, while the bulk hydrogen and oxygen emission share a common kinematic
  imprint within an inner, denser region.\r\n\r\n5.3. Line Kinematics\r\nBefore we
  proceed to discussing the individual features in more detail, we would like to comment
  on the systematic velocity offsets between various line species in the spectrum
  of GLIMPSE-17775. As mentioned previously, we choose the redshift of the narrow
  forbidden [S iii] λ9701 as the systemic reference, due to it being relatively bright
  and isolated. We place all velocity offsets in context by plotting all values from
  Tables 4 and 5 in Figure 7.\r\n\r\nZoom InZoom OutReset image size\r\nFigure 7.
  Velocity offsets (relative to [S iii]λ9071) and FWHM for all detected lines. Narrow
  permitted lines are shown as maroon circles (open for forbidden), broad lines as
  blue, absorption as gold, and Fe ii lines as green diamonds. The shaded band marks
  the velocity uncertainty set by the median spectral resolution. Narrow lines align
  closely with the systemic redshift, while absorption features show moderate blueshifts
  of ∼150 km s−1.\r\n\r\nDownload figure:\r\n\r\nStandard imageHigh-resolution image\r\nWhile
  every fit formally yields a centroid, the significance of any offset is constrained
  by the spectral resolution and S/N of the data. To gauge which velocity shifts are
  meaningful, we adopt a conservative uncertainty of ΔV ∼ med(R)/5, with R = λ/Δλ.
  This corresponds to ∼60 km s−1, below which offsets are unlikely to be statistically
  significant.\r\n\r\nQualitatively, we do not find systematic shifts of either permitted
  or forbidden narrow lines relative to the systemic redshift. Iron lines also appear
  consistent with the systemic velocity. In contrast, the permitted broad lines, together
  with their associated absorption components, show a consistent blueshift of order
  ∼100 km s−1.\r\n\r\nSuch blueshifts are commonly interpreted as signatures of outflowing
  gas in the BLR, where scattering and absorption occur preferentially along outflowing
  sight lines. In the context of GLIMPSE-17775, this modest but systematic offset
  strengthens the case for a stratified cocoon, while the narrow lines trace gas in
  the outer regions at systemic velocity, the BLR and absorbing layers appear to be
  participating in bulk outflows. Confirming the detailed velocity structure, however,
  will require higher-resolution follow-up with the NIRSpec H-gratings (e.g., A. Saldana-Lopez
  et al. 2025; A. Torralba et al. 2026).\r\n\r\n5.4. Hydrogen Absorption Lines\r\nAlthough
  no strong hydrogen absorption lines are explicitly detected, the Hα profile (Figure
  2) shows a noticeable asymmetry, with suppressed flux on the blue side of the line.
  This feature is best modeled by a blueshifted (∼−200 km s−1) absorption component,
  as already noted in Section 4. Similar nonresonant absorption signatures (e.g.,
  Balmer lines) are now routinely observed in LRDs across a wide range of redshifts
  (e.g., J. E. Greene et al. 2024; V. Kokorev et al. 2024b; I. Labbe et al. 2024;
  X. Lin et al. 2024; A. J. Taylor et al. 2025). The presence of such absorption implies
  high gas densities of order n ∼ 109 cm−3 (P. B. Hall 2007; K. Inayoshi & R. Maiolino
  2025). Interestingly, only atoms in the n = 2 state appear significantly populated,
  as we detect no evidence for Paschen absorption in any of the five lines present
  in our spectrum. This is not an instrumental effect of the M-grating, as we clearly
  detect an absorption feature in He i λ10830 but not in the immediately adjacent
  Paγ. This indicates that the n = 3 state is comparatively underpopulated.\r\n\r\nAnother
  key manifestation of the same physical mechanism is the Balmer break, corresponding
  to the n = ∞ → n = 2 transition limit. A prominent break is common in many LRD spectra
  (D. J. Setton et al. 2025), though not ubiquitous (e.g., V. Kokorev et al. 2023;
  R. Tripodi et al. 2025). While our spectral coverage does not extend to the Balmer
  limit itself, we observe a discontinuity of ∼1 mag between the F200W and F150W filters.
  Due to the F200W coverage of the SED, this flux jump cannot be attributed to line
  boosting from Hβ and the [O iii] doublet. Adopting the break parameterization of
  R. P. Naidu et al. (2025), we use our best-fit SED and measure fν,4050Å/fν,3670Å
  = 2.02 ± 0.10. Although weaker than the extreme values (∼4–7) reported for LRDz9
  (A. J. Taylor et al. 2025), MoM BH*-1 (R. P. Naidu et al. 2025), or “the Cliff”
  (A. de Graaff et al. 2025b), this value lies close to the maximum achievable by
  evolved stellar populations (I. Labbe et al. 2024; B. Wang et al. 2024). However,
  this measurement is based on the total (PS+host) photometry. Given that the UV continuum
  is spatially resolved, as we have shown in Section 4.1, host-galaxy contamination
  may dilute the intrinsic break strength of the central component. While uncertainties
  on the PS/host decomposition increase significantly toward the rest-optical, we
  find that using the PS-only photometry produces a noticeably sharper break, increasing
  the inferred strength by ∼30%–50% to fν,4050Å/fν,3670Å ≈ 2.6–3.0. Although this
  does not allow us to robustly conclude whether the intrinsic PS break reaches the
  most extreme BH*-type objects (A. de Graaff et al. 2025b; R. P. Naidu et al. 2025;
  A. J. Taylor et al. 2025), it suggests that the Balmer discontinuity becomes stronger
  once the host contribution is removed, consistent with recent findings that host
  light can suppress the apparent break amplitude (e.g., A. de Graaff et al. 2025d;
  W. Q. Sun et al. 2026).\r\n\r\nTaken together, the presence of asymmetry in the
  Hα profile, likely caused by blueshifted Balmer absorption, and a Balmer break adds
  to the evidence, complementing the exponential line wings, that the emission in
  GLIMPSE-17775 arises from a dense, ionized cocoon of gas. The lack of a detectable
  Paschen break is consistent with this picture, as high densities and optical depths
  result in Thomson scattering while also naturally washing out higher-order continuum
  edges (e.g., B. Wang et al. 2025). Assuming LTE, an extremely low ratio n3/n2 ≲
  0.01 corresponds to an electron temperature of Te ∼ 5000 K or below, consistent
  with the warm, partially ionized gas expected in dense LRD cocoons.\r\n\r\nWe also
  observe moderately prominent and extremely prominent blueshifted absorption, respectively,
  in He i λ7065 and He i λ10830. The mechanism for this is similar, but not identical
  to, the hydrogen lines. We also note the prominent blueshifted absorption seen in
  both He i λ7065 and He i λ10830. However, the physical mechanism driving these helium
  features differs fundamentally from that of the hydrogen lines; we return to this
  in the following section.\r\n\r\n5.5. Helium Lines\r\nBoth He i λ7065 and He i λ10830
  show blueshifted (∼70−80 km s−1 from the narrow-line center) absorption components
  with widths of ∼600−700 km s−1. Unlike the Balmer series, helium transitions are
  resonantly scattered, so the arguments regarding n = 2 state abundances do not apply.
  Before addressing the absorption itself, it is useful to consider what the observed
  line strengths already tell us.\r\n\r\nIn the spectrum of GLIMPSE-17775, we detect
  three He i lines: λ6680, λ7065, and λ10830. These originate from different physical
  mechanisms. The λ6680 singlet line is produced via recombination or radiative pumping,
  and is only weakly dependent on density. By contrast, λ7065 and λ10830 belong to
  the triplet system (along with λ3889, not covered by G395M), where the lower level
  is populated due to its very long lifetime. Electrons in this “ground state” can
  be collisionally or radiatively excited into higher energies, and therefore the
  triplet-line strengths depend strongly on density and, to a lesser extent, temperature.
  As emphasized by D. A. Berg et al. (2026), He i λ10830 is the most sensitive density
  diagnostic among these transitions, followed by λ7065. The fact that both are much
  stronger than λ6680 indicates that the region where they form is very dense. The
  prominence of λ10830 in particular already points to a high-density environment
  with a temperature T ≳ 104 K. Further, the broad λ6680 line has a noticeably larger
  FWHM than the triplet lines but is consistent with hydrogen recombination lines,
  which again makes sense since both originate from the same mechanism.\r\n\r\nWhat
  about absorption? Its presence further reinforces this picture. The lower level
  (23S) of the triplet system is a metastable, long-lived state that effectively acts
  as a ground state in dense or partially ionized gas. As a result, photons from the
  23P → 23S transition can be resonantly absorbed and reemitted many times, analogous
  to Lyα or Mg ii. This mechanism naturally produces strong absorption features when
  the He i column density is high. The fact that He i λ10830 not only dominates the
  helium spectrum in emission but also shows the deepest absorption in the entire
  spectrum provides compelling evidence for a dense, ionized cocoon of gas enshrouding
  GLIMPSE-17775.\r\n\r\n5.6. Oxygen Lines\r\nAbove, we noted that O i λ8446 and λ11290
  share very similar profiles with the hydrogen recombination lines. This is naturally
  expected because neutral oxygen is tightly coupled to hydrogen via charge exchange,
  which rapidly equilibrates the O/H ionization states in dense gas. When charge exchange
  is fast (high nH), the O i/O ii ratio tracks the H i/H ii ratio, so the O i-emitting
  gas shares the same kinematics as the hydrogen recombination region (B. T. Draine
  2011). The observed agreement in FWHM between H and O i lines is therefore an important
  consistency check that both species originate in the same dense, partially ionized
  phase.\r\n\r\nA second, independent clue of high gas density and radiation field
  intensity comes from the excitation mechanism. The O iλ8446–λ11287 pair is the classic
  signature of Lyβ (Bowen) fluorescence: Lyβ pumps O i from the ground state and the
  ensuing cascade preferentially populates the levels that emit at 1.129 μm, which
  then cascade down through the 8446 Å line. In this channel, the line emissivity
  scales with both the neutral oxygen (or equivalently neutral hydrogen, via charge
  exchange) column and the local Lyβ radiation field. Therefore, producing strong
  O i fluorescence requires both a very bright Lyβ source and a dense neutral (or
  partially ionized) cocoon.\r\n\r\nFurther, we do not detect (5σ upper limit <12/[10−20
  erg s−1 cm−2]) any of the other permitted O iλ7774, λ7254, and λ7790 lines, and
  the [O i] λ6302/O i λ8446 ratio is weak. If collisional excitation or pure recombination
  dominated, these lines would be comparatively strong; their absence strongly favors
  Bowen fluorescence as the primary driver of the observed O i emission.\r\n\r\nFinally,
  the velocity structure adds a natural stratification: hydrogen recombination and
  O i (fluorescent, charge-exchange coupled) share similar widths and profiles, while
  He i lines are systematically narrower. Since He i triplet transitions emerge from
  a metastable 23S level (with distinct, density-sensitive population pathways and
  resonant transfer), they likely trace a kinematically distinct layer within the
  same cocoon.\r\n\r\n5.7. Lyα Fluorescence in Iron Lines\r\nPermitted iron emission,
  primarily Fe ii and Fe iii (e.g., I. Labbe et al. 2024; R. Tripodi et al. 2025;
  A. Torralba et al. 2026), but in some cases extending to highly ionized species
  such as Fe vii (E. Lambrides et al. 2025; M. Tang et al. 2025) and Fe x (L. J. Furtak
  et al. 2024), has become a recurring feature in LRD spectra. In GLIMPSE-17775, the
  spectrum is exceptionally rich in NIR iron lines; we identify 16 Fe ii and one Fe
  iii transition. Understanding the origin of this emission is key to interpreting
  the dense-gas environment in LRDs.\r\n\r\nThe physics of Fe ii emission has long
  been a challenge for BLR photoionization models (M. Joly 1993). Thick, high-column-density
  (∼1025 cm−2) gas at the edges of the accretion disk has been invoked as a potential
  source (M. Joly 1987; S. Collin-Souffrin et al. 1988), where the scattering and
  absorption of the hard X-ray photons ionize the gas. Similarly, this would also
  enhance the Balmer and Paschen line luminosities. Further, extensive theoretical
  work has shown that Lyα fluorescence is fundamental in reproducing the observed
  Fe ii strengths (T. A. A. Sigut & A. K. Pradhan 1998, 2003). Lyα pumping not only
  boosts the UV and optical Fe ii emission, but also predicts strong lines in the
  NIR.\r\n\r\nThis expectation aligns closely with our observations. In Figure 8,
  we compare our measured Fe ii flux ratios (normalized to Fe ii λ9075) against the
  Lyα-pumped model predictions of T. A. A. Sigut & A. K. Pradhan (2003). With the
  exception of Fe ii λ9179, affected by blending with Fe ii λ9204 and Pa9, we find
  remarkably good agreement across the suite of detected features. In particular,
  the dense forest of Fe ii transitions spanning λλ9000–9200 (center-right panel in
  Figure 2) is reproduced almost exactly by the theoretical spectrum (see Figure 11
  in T. A. A. Sigut & A. K. Pradhan 2003). We overlay the T. A. A. Sigut & A. K. Pradhan
  (2003) model directly on our continuum-subtracted fit in Figure 8, demonstrating
  that the observed Fe ii emission is fully consistent with fluorescence in dense
  gas near the BLR. The implication is that the majority of the Fe ii emission in
  GLIMPSE-17775 arises through Lyα pumping, directly tracing an extremely dense medium,
  ionized by an extremely luminous source, likely an accreting black hole. Given that
  the Fe ii lines are somewhat narrower than other permitted features, it is likely
  that the emitting region is located farther from the BLR—something that has already
  been shown in a classic example of a narrow Fe ii emitter, I Zw 1 (R. J. Rudy et
  al. 2000; A. O. M. Marinello et al. 2016).\r\n\r\nZoom InZoom OutReset image size\r\nFigure
  8. Lyα-pumped iron emission in GLIMPSE-17775. Left: observed Fe ii flux ratios (black
  points), normalized to Fe iiλ9075, compared with predictions from Lyα fluorescence
  models of T. A. A. Sigut & A. K. Pradhan (2003, blue). The close correspondence
  across ∼14 lines indicates a common excitation mechanism driven by Lyα pumping in
  dense, partially shielded gas. Right: zoom in on the λλ9000–9400 complex, showing
  the remarkable agreement between the modeled continuum-subtracted Fe ii spectrum
  (black) and the T. A. A. Sigut & A. K. Pradhan (2003) model (blue). We show air
  wavelengths of each Fe ii line directly from T. A. A. Sigut & A. K. Pradhan (2003),
  including the blended features. Together, these comparisons support an origin in
  the dense inner regions of the cocoon surrounding the accreting black hole.\r\n\r\nDownload
  figure:\r\n\r\nStandard imageHigh-resolution image\r\nTogether with the Balmer absorption,
  helium triplet features, and Bowen fluorescence in O i, the iron forest adds another
  piece of evidence that points to a dense cocoon enshrouding the black hole.\r\n\r\n5.8.
  Source Properties\r\nBased on the previous discussion, we now present the likely
  physical properties of the black hole and its host. The coexistence of broad permitted
  and narrow forbidden lines indicates, as in most LRDs (R. E. Hviding et al. 2025),
  that the broad components originate in an AGN BLR. Following J. E. Greene & L. C.
  Ho (2005), we derive MBH from the luminosity and width of the broad Hα line, assuming
  the exponential-wing profile demonstrated in Figures 2 and 5. With a FWHMHα = 1024
  ± 21 km s−1, negligible dust, and μ = 2.04, we obtain , where the dominant uncertainty
  arises from the J. E. Greene & L. C. Ho (2005) calibration. A purely Gaussian fit,
  though statistically disfavored, would yield a FWHM 3 times larger and a black hole
  mass nearly a dex higher. Throughout this work, we adopt the MBH from the exponential
  model.\r\n\r\nFurther, by assuming that the bolometric luminosity (Lbol) scales
  as Lbol = 130 × LHα (G. T. Richards et al. 2006), we find Lbol = (1.06 ± 0.14) ×
  1045 erg s–1. Using our MBH derived by assuming exponential wings, we find that
  this object is accreting at a super-Eddington rate, Lbol/Ledd = 1.86 ± 0.25. This
  is higher than the vast majority of LRDs at all redshifts (e.g., V. Kokorev et al.
  2023; L. J. Furtak et al. 2024; I. Juodžbalis et al. 2024; R. Maiolino et al. 2024;
  H. B. Akins et al. 2025b; D. D. Kocevski et al. 2025; A. J. Taylor et al. 2025),
  found to accrete at sub-Eddington rates. However, recent works examining LRDs with
  extreme Balmer breaks derive accretion rates that exceed the Eddington limit (E.
  Lambrides et al. 2024; A. de Graaff et al. 2025b; R. P. Naidu et al. 2025).\r\n\r\nA
  recent work examining multiwavelength LRD data suggests that the bolometric luminosity
  emerges predominantly from the rest-frame optical, with X-ray and radio contributions
  being largely subdominant (J. E. Greene et al. 2026). Given the suggested dominance
  of optical light in LRDs, the much lower bolometric corrections (×7–10 lower) would
  imply lower black hole masses and total bolometric luminosities (e.g., those derived
  from Hα) than standard AGN prescriptions (e.g., J. E. Greene & L. C. Ho 2005) might
  suggest. This adjustment would lower both the inferred black hole masses and bolometric
  luminosities. Because these two quantities scale together, the implied super-Eddington
  nature of GLIMPSE-17775 would remain unchanged, although the black hole mass could
  decrease to ∼105.5–105.8M⊙. This interpretation is consistent with dense-gas (BH*)
  models, which generically predict Eddington or super-Eddington accretion in heavily
  obscured environments (e.g., D. Kido et al. 2025; H. Liu et al. 2025; A. Sneppen
  et al. 2026). A more detailed reassessment of bolometric corrections for LRDs is
  clearly warranted, but such an analysis lies beyond the scope of this work. For
  consistency with previous studies, we adopt standard AGN bolometric corrections
  throughout, with all derived parameters listed in Table 1.\r\n\r\nFinally, we estimate
  an upper limit on the stellar mass in GLIMPSE-17775. Previous studies have modeled
  LRDs using joint galaxy+AGN SED decomposition (e.g., V. Kokorev et al. 2023; L.
  J. Furtak et al. 2024), and more recently, within the BH* framework, have assumed
  that most of the rest-UV flux arises from the host galaxy (R. P. Naidu et al. 2025;
  A. J. Taylor et al. 2025). Our spatial decomposition (Figure 4) supports this assumption:
  The extended component contributes >80% of the rest-UV light, implying that the
  bulk of the stellar mass resides in this resolved structure. Given this, we adopt
  a simple empirical approach using the MUV–M* relation (e.g., D. P. Stark et al.
  2009; I. Labbé et al. 2013) and obtain a conservative upper limit on the stellar
  mass of M* ≲ 107.5M⊙. This in turn gives us a black hole-to-host mass ratio of ≲0.14,
  which is significantly elevated from local expectations (J. E. Greene & L. C. Ho
  2005), but is not as extreme as some other LRDs reported in the literature (V. Kokorev
  et al. 2023; L. J. Furtak et al. 2024; R. Maiolino et al. 2024).\r\n\r\n6. Discussion
  and Summary\r\n6.1. Dense and Ionized Gas Surrounding the AGN\r\nOur NIRSpec G395M
  observations of GLIMPSE-17775 reveal a remarkably consistent picture: Across independent
  tracers, the line emission requires an environment of extremely high density and
  partial ionization.\r\n\r\nFirst, the broad permitted lines are universally better
  fit by exponential wings, a hallmark of electron scattering in gas with ne ≳ 108
  cm−3 and column densities approaching Ne ∼ 1024 cm−2. Such profiles are not reproduced
  by Doppler broadening alone and point to an ionized scattering medium enveloping
  the source. The fact that hydrogen and O i lines share consistent FWHM values further
  anchors this interpretation, as charge exchange tightly couples neutral oxygen to
  the ionization and kinematics of hydrogen.\r\n\r\nSecond, the detection of blueshifted
  Balmer absorption and a significant Balmer break both require high n = 2 populations
  and densities n ∼ 109 cm−3. Helium transitions provide a complementary view: The
  triplet lines λ7065 and λ10830 are both strongly enhanced relative to the singlet
  states and show deep blueshifted absorption, consistent with resonant scattering
  from the metastable 23S level. Their systematically narrower widths compared to
  hydrogen and oxygen suggest stratification, with helium arising from denser, more
  compact layers of the cocoon.\r\n\r\nThird, the O i λ8446–λ11290 pair confirms Lyβ
  fluorescence, requiring both a bright Lyβ radiation field and a dense reservoir
  of neutral gas. The absence of other permitted O i lines not fed by Lyβ strengthens
  this conclusion. Finally, the detection of 16 Fe ii lines, forming an incredibly
  rich iron forest in this LRD, matches predictions from Lyα fluorescence models,
  again demanding an intense radiation field and very high densities.\r\n\r\nBecause
  the BLR is unresolved in essentially all AGN, broad-line widths are traditionally
  interpreted as virial tracers of the black hole potential. In GLIMPSE-17775, the
  virial story alone is insufficient: The issue is not how broad the lines are, but
  how they broaden. The profiles exhibit extended, nearly linear wings in velocity
  space that are incompatible with a Gaussian. Instead, the lines are systematically
  and significantly better described by a model consisting of a narrow Gaussian core
  (virial motion) plus exponential wings, the hallmark of Thomson scattering in a
  dense ionized medium. Thus, the line shape encodes both gravitational kinematics
  and radiative-transfer physics in the surrounding cocoon. Our schematic (Figure
  9) summarizes this revised view: In LRDs, broad-line profiles are not set by dynamics
  alone, but by the scattering environment through which the photons escape.\r\n\r\nZoom
  InZoom OutReset image size\r\nFigure 9. Physical picture of the dense cocoon around
  GLIMPSE-17775. The inner region (1) corresponds to the dense, highly ionized broad-line
  region (BLR) where electron scattering (orange lines) produces exponential wings,
  H and O I share coupled kinematics (via charge exchange and Bowen fluorescence),
  and strong Balmer absorption/break signatures arise. The outer layer (2) represents
  an intermediate-density ionized medium, where He I triplet lines show resonant absorption
  from the metastable 23S level and Fe II emission is driven by Lyα fluorescence.
  Together, these zones form a stratified cocoon enshrouding the accreting black hole.
  The bottom-right panel shows stacked line profiles of H, O i, He i, and Fe ii.\r\n\r\nDownload
  figure:\r\n\r\nStandard imageHigh-resolution image\r\nSuch conditions—high optical
  depths, large column densities, and evidence for radiation-dominated gas—are precisely
  those expected in super-Eddington accretion flows. In this regime, radiation pressure
  inflates the inner accretion structure, driving powerful winds and forming the very
  dense, partially ionized envelope we infer here. The low X-ray luminosities and
  weak radio emission commonly observed in LRDs (e.g., T. T. Ananna et al. 2024; M.
  Yue et al. 2024; H. B. Akins et al. 2025a; M. Kokubo & Y. Harikane 2025) are consistent
  with this picture: The X-rays are likely absorbed or thermalized within the optically
  thick cocoon, while dust cannot survive in such an intense radiation field (e.g.,
  E. Lambrides et al. 2024; A. de Graaff et al. 2025b; K. Inayoshi & R. Maiolino 2025;
  R. P. Naidu et al. 2025; A. J. Taylor et al. 2025). Thus, the spectroscopic signatures
  observed in GLIMPSE-17775—exponential wings, absorption features, and fluorescence-driven
  metal lines—fit naturally into a scenario where super-Eddington accretion onto a
  low-mass black hole powers the luminous yet heavily reprocessed emission.\r\n\r\nTaken
  together, the exponential wings, Balmer and helium absorption, Bowen oxygen lines,
  and Lyα-pumped iron forest all converge on the same physical picture: GLIMPSE-17775
  is enshrouded in a dense, partially ionized cocoon of gas.\r\n\r\n6.2. Final Remarks\r\nUsing
  a combination of the intrinsically deepest NIRCam photometry and NIRSpec G395M observations
  of the lensed AS1063 field, we present a detailed investigation of a LRD at z =
  3.501. The spectrum of GLIMPSE-17775 is exceptionally rich, with more than 40 detected
  features, allowing us to probe the physical conditions of the gas with unprecedented
  detail. Multiple independent diagnostics converge on the presence of a dense, partially
  ionized cocoon heated by a powerful ionizing source.\r\n\r\nTypical of other LRDs,
  GLIMPSE-17775 is extremely compact in the rest-optical (reff < 300 pc) but exhibits
  more extended structure in the rest-UV (reff ∼ 1000 pc; Figure 1). It shows unmistakable
  AGN signatures through broad permitted lines (e.g., D. D. Kocevski et al. 2023;
  V. Kokorev et al. 2023; J. E. Greene et al. 2024; L. J. Furtak et al. 2024). The
  uniquely deep G395M spectrum further reveals clues to the physical origin of both
  its continuum and line-emission properties: We detect exponential broad-line wings,
  Balmer and helium absorption, Bowen-pumped O i, Fe ii emission produced by Lyα fluorescence,
  and evidence for rapid, potentially super-Eddington growth.\r\n\r\nTogether, these
  diagnostics provide one of the clearest cases yet for the BH* “dense cocoon” scenario
  (A. de Graaff et al. 2025b; K. Inayoshi & R. Maiolino 2025; R. P. Naidu et al. 2025;
  A. J. Taylor et al. 2025). The same ingredients we observe—exponential broad wings,
  Balmer-break absorption, He i absorption, and rich Fe ii and O i fluorescence—have
  been detected individually in several other bright LRDs with medium- and high-resolution
  spectroscopy (e.g., L. J. Furtak et al. 2024; I. Juodžbalis et al. 2024; I. Labbe
  et al. 2024; F. D’Eugenio et al. 2025; E. Lambrides et al. 2025; B. Wang et al.
  2025; A. Torralba et al. 2026), suggesting that dense, optically thick gas may be
  a common feature of the population rather than an anomaly. What distinguishes GLIMPSE-17775
  is that all signatures are captured simultaneously and at high S/N, allowing a self-consistent
  physical interpretation. If such cocoons are widespread, then super-Eddington accretion
  may be a typical pathway for black hole growth in LRDs, especially among the most
  luminous systems. Establishing how these signatures vary with luminosity and redshift
  will be essential for determining whether dense cocoons represent a dominant mode
  of early black hole assembly.\r\n\r\nThe convergence of five independent diagnostics—exponential
  scattering wings, Balmer-limit absorption, helium triplet physics, and two distinct
  fluorescence channels—leaves little doubt: GLIMPSE-17775 hosts a dense (n ∼ 108−9
  cm−3), optically thick (Ne ∼ 1024 cm−2) cocoon of partially ionized gas surrounding
  a super-Eddington accreting black hole. This represents some of the most direct
  and comprehensive spectroscopic evidence to date for the dense cocoon scenario in
  LRDs.\r\n\r\nAcknowledgments\r\nThe authors would like to thank Aaron Sigut and
  Anil Pradhan for their help with understanding iron emission in active galactic
  nuclei. The authors would like to acknowledge the National Institute of Standards
  and Technology (NIST) database of spectral lines (A. Kramida et al. 2024), which
  made identification of less-known emission features possible. V.K., J.C., S.F.,
  D.B., L.F., T.H., and J.M. acknowledge support from the University of Texas at Austin
  Cosmic Frontier Center. A.Z. acknowledges support by the Israel Science Foundation
  grant No. 864/23. This work is based on observations made with the NASA/ESA/CSA
  James Webb Space Telescope, obtained at the Space Telescope Science Institute, which
  is operated by the Association of Universities for Research in Astronomy, Incorporated,
  under NASA contract NAS5-03127. The JWST data presented in this article were obtained
  from the Mikulski Archive for Space Telescopes (MAST) at the Space Telescope Science
  Institute. The specific observations analyzed can be accessed via doi:10.17909/4byn-fe55
  and doi:10.17909/zq0c-8t87. These observations are associated with programs GO #3293
  and DDT #9223.\r\n\r\nFacilities: JWST - James Webb Space Telescope, HST - Hubble
  Space Telescope satellite.\r\n\r\nSoftware: EAZY (G. B. Brammer et al. 2008), grizli
  (G. Brammer 2023), msaexp (G. Brammer 2022), photutils (L. Bradley et al. 2020),
  pysersic (I. Pasha & T. B. Miller 2023), sep (K. Barbary 2016), SExtractor (E. Bertin
  & S. Arnouts1996)."
article_number: '153'
article_processing_charge: Yes
article_type: original
arxiv: 1
author:
- first_name: Vasily
  full_name: Kokorev, Vasily
  last_name: Kokorev
- first_name: John
  full_name: Chisholm, John
  last_name: Chisholm
- first_name: Rohan P.
  full_name: Naidu, Rohan P.
  last_name: Naidu
- first_name: Seiji
  full_name: Fujimoto, Seiji
  last_name: Fujimoto
- first_name: Hakim
  full_name: Atek, Hakim
  last_name: Atek
- first_name: Gabriel
  full_name: Brammer, Gabriel
  last_name: Brammer
- first_name: Steven L.
  full_name: Finkelstein, Steven L.
  last_name: Finkelstein
- first_name: Hollis B.
  full_name: Akins, Hollis B.
  last_name: Akins
- first_name: Danielle A.
  full_name: Berg, Danielle A.
  last_name: Berg
- first_name: Lukas J.
  full_name: Furtak, Lukas J.
  last_name: Furtak
- first_name: Qinyue
  full_name: Fei, Qinyue
  last_name: Fei
- first_name: Tiger Yu-Yang
  full_name: Hsiao, Tiger Yu-Yang
  last_name: Hsiao
- first_name: Ivo
  full_name: Labbé, Ivo
  last_name: Labbé
- first_name: Jorryt J
  full_name: Matthee, Jorryt J
  id: 7439a258-f3c0-11ec-9501-9df22fe06720
  last_name: Matthee
  orcid: 0000-0003-2871-127X
- first_name: Julian B.
  full_name: Muñoz, Julian B.
  last_name: Muñoz
- first_name: Pascal A.
  full_name: Oesch, Pascal A.
  last_name: Oesch
- first_name: Richard
  full_name: Pan, Richard
  last_name: Pan
- first_name: Pierluigi
  full_name: Rinaldi, Pierluigi
  last_name: Rinaldi
- first_name: Alberto
  full_name: Saldana-Lopez, Alberto
  last_name: Saldana-Lopez
- first_name: Daniel
  full_name: Schaerer, Daniel
  last_name: Schaerer
- first_name: Marta
  full_name: Volonteri, Marta
  last_name: Volonteri
- first_name: Adi
  full_name: Zitrin, Adi
  last_name: Zitrin
citation:
  ama: Kokorev V, Chisholm J, Naidu RP, et al. The Deepest GLIMPSE of a dense gas
    cocoon enshrouding a Little Red Dot. <i>The Astrophysical Journal</i>. 2026;1004(2).
    doi:<a href="https://doi.org/10.3847/1538-4357/ae4ed7">10.3847/1538-4357/ae4ed7</a>
  apa: Kokorev, V., Chisholm, J., Naidu, R. P., Fujimoto, S., Atek, H., Brammer, G.,
    … Zitrin, A. (2026). The Deepest GLIMPSE of a dense gas cocoon enshrouding a Little
    Red Dot. <i>The Astrophysical Journal</i>. IOP Publishing. <a href="https://doi.org/10.3847/1538-4357/ae4ed7">https://doi.org/10.3847/1538-4357/ae4ed7</a>
  chicago: Kokorev, Vasily, John Chisholm, Rohan P. Naidu, Seiji Fujimoto, Hakim Atek,
    Gabriel Brammer, Steven L. Finkelstein, et al. “The Deepest GLIMPSE of a Dense
    Gas Cocoon Enshrouding a Little Red Dot.” <i>The Astrophysical Journal</i>. IOP
    Publishing, 2026. <a href="https://doi.org/10.3847/1538-4357/ae4ed7">https://doi.org/10.3847/1538-4357/ae4ed7</a>.
  ieee: V. Kokorev <i>et al.</i>, “The Deepest GLIMPSE of a dense gas cocoon enshrouding
    a Little Red Dot,” <i>The Astrophysical Journal</i>, vol. 1004, no. 2. IOP Publishing,
    2026.
  ista: Kokorev V, Chisholm J, Naidu RP, Fujimoto S, Atek H, Brammer G, Finkelstein
    SL, Akins HB, Berg DA, Furtak LJ, Fei Q, Hsiao TY-Y, Labbé I, Matthee JJ, Muñoz
    JB, Oesch PA, Pan R, Rinaldi P, Saldana-Lopez A, Schaerer D, Volonteri M, Zitrin
    A. 2026. The Deepest GLIMPSE of a dense gas cocoon enshrouding a Little Red Dot.
    The Astrophysical Journal. 1004(2), 153.
  mla: Kokorev, Vasily, et al. “The Deepest GLIMPSE of a Dense Gas Cocoon Enshrouding
    a Little Red Dot.” <i>The Astrophysical Journal</i>, vol. 1004, no. 2, 153, IOP
    Publishing, 2026, doi:<a href="https://doi.org/10.3847/1538-4357/ae4ed7">10.3847/1538-4357/ae4ed7</a>.
  short: V. Kokorev, J. Chisholm, R.P. Naidu, S. Fujimoto, H. Atek, G. Brammer, S.L.
    Finkelstein, H.B. Akins, D.A. Berg, L.J. Furtak, Q. Fei, T.Y.-Y. Hsiao, I. Labbé,
    J.J. Matthee, J.B. Muñoz, P.A. Oesch, R. Pan, P. Rinaldi, A. Saldana-Lopez, D.
    Schaerer, M. Volonteri, A. Zitrin, The Astrophysical Journal 1004 (2026).
das_tickbox: '1'
dataavailabilitystatement: "The specific observations analyzed can be accessed via
  doi:10.17909/4byn-fe55 and doi:10.17909/zq0c-8t87. These observations are associated
  with programs GO #3293 and DDT #9223.\r\n\r\nFacilities: JWST - James Webb Space
  Telescope, HST - Hubble Space Telescope satellite.\r\n\r\nSoftware: EAZY (G. B.
  Brammer et al. 2008), grizli (G. Brammer 2023), msaexp (G. Brammer 2022), photutils
  (L. Bradley et al. 2020), pysersic (I. Pasha & T. B. Miller 2023), sep (K. Barbary
  2016), SExtractor (E. Bertin & S. Arnouts1996)."
date_created: 2026-07-13T09:48:38Z
date_published: 2026-06-10T00:00:00Z
date_updated: 2026-07-13T13:25:09Z
day: '10'
ddc:
- '520'
department:
- _id: JoMa
doi: 10.3847/1538-4357/ae4ed7
external_id:
  arxiv:
  - '2511.07515'
file:
- access_level: open_access
  checksum: 464e60013bf14d087eb0968e9c81a269
  content_type: application/pdf
  creator: dernst
  date_created: 2026-07-13T13:23:11Z
  date_updated: 2026-07-13T13:23:11Z
  file_id: '22313'
  file_name: 2026_AstrophysicalJour_Kokorev.pdf
  file_size: 2435643
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  success: 1
file_date_updated: 2026-07-13T13:23:11Z
has_accepted_license: '1'
intvolume: '      1004'
issue: '2'
language:
- iso: eng
month: '06'
oa: 1
oa_version: Published Version
publication: The Astrophysical Journal
publication_identifier:
  eissn:
  - 1538-4357
  issn:
  - 0004-637X
publication_status: published
publisher: IOP Publishing
quality_controlled: '1'
researchdata_availability: no
scopus_import: '1'
status: public
supplementarymaterial: no
title: The Deepest GLIMPSE of a dense gas cocoon enshrouding a Little Red Dot
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 1004
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '22297'
abstract:
- lang: eng
  text: 'Determination of the rheological properties of cells is known to require
    active measurements, which largely depend on the internalization of mechanical
    probes. Here, we circumvent this problem via the introduction of Rheological focused
    light-induced cytoplasmic streaming (Rheo-FLUCS): an active, yet probe-free approach
    that leverages light-induced flows to access mechanical changes in complex systems.
    While Rheo-FLUCS is facilitated by thermoviscous expansion phenomena rather than
    external forces, here we show equivalence in its ability to measure relative viscoelastic
    properties. Specifically, we demonstrate a phase-lag equivalence with probe-dependent
    active microrheology in a wide range of physically different, yet chemically identical
    materials. We exemplify the utility of Rheo-FLUCS in three distinctly different
    biological systems: compound-treated mouse fibroblasts (NIH-3T3), genetically
    modified human osteoblasts (U2OS) to elucidate the role of myosins in cytoplasmic
    mechanics, and early ascidian oocytes of Phallusia mammillata at fertilization
    stage. Our biological use-cases exemplify the application versatility of Rheo-FLUCS,
    which in the future may use phase information as a marker for developmental success.'
acknowledgement: The authors gratefully acknowledge help from Dr. Benjamin Seelbinder,
  Mr. Claudius George, and Mr. Falk Elsner in designing and constructing the magnetic
  needle for force-driven rheology experiments. We thank Dr. Iain Patten for valuable
  discussions on the structure of the manuscript and Mr. Ivan Saraev for graphics
  support. I.D.S. and M.K. kindly acknowledge funding from the Life grant by Volkswagen
  Foundation (Life! grant no. 92772), Deutsche Forschungsgemeinschaft (DFG, German
  Research Foundation, Germany's Excellence Strategy, 2082/1 and grant no. 515462906),
  and the Hector Foundation. I.D.S. was additionally funded by the Karlsruhe Institute
  of Technology (Excellence Strategy via the Young Investigator Group Preparation
  Program). V.R.K., S.W., and M.K. thank the ERC Starting Grant GHOSTs (grant no.
  853619).
article_number: pgag190
article_processing_charge: Yes
article_type: original
author:
- first_name: Iliya D
  full_name: Stoev, Iliya D
  last_name: Stoev
- first_name: Madison
  full_name: Bolger-Munro, Madison
  id: 516F03FA-93A3-11EA-A7C5-D6BE3DDC885E
  last_name: Bolger-Munro
  orcid: 0000-0002-8176-4824
- first_name: Antonio
  full_name: Minopoli, Antonio
  last_name: Minopoli
- first_name: Susan
  full_name: Wagner, Susan
  last_name: Wagner
- first_name: Venkat Raghavan
  full_name: Krishnaswamy, Venkat Raghavan
  last_name: Krishnaswamy
- first_name: Elena
  full_name: Erben, Elena
  last_name: Erben
- first_name: Kai
  full_name: Weißenbruch, Kai
  last_name: Weißenbruch
- first_name: Nicola
  full_name: Maghelli, Nicola
  last_name: Maghelli
- first_name: Martin
  full_name: Bastmeyer, Martin
  last_name: Bastmeyer
- first_name: Carl-Philipp J
  full_name: Heisenberg, Carl-Philipp J
  id: 39427864-F248-11E8-B48F-1D18A9856A87
  last_name: Heisenberg
  orcid: 0000-0002-0912-4566
- first_name: Moritz
  full_name: Kreysing, Moritz
  last_name: Kreysing
biorxivid: 1
citation:
  ama: Stoev ID, Bolger-Munro M, Minopoli A, et al. Active and probe-free intracellular
    rheology via phase-sensitive thermoviscous flows. <i>PNAS Nexus</i>. 2026;5(6).
    doi:<a href="https://doi.org/10.1093/pnasnexus/pgag190">10.1093/pnasnexus/pgag190</a>
  apa: Stoev, I. D., Bolger-Munro, M., Minopoli, A., Wagner, S., Krishnaswamy, V.
    R., Erben, E., … Kreysing, M. (2026). Active and probe-free intracellular rheology
    via phase-sensitive thermoviscous flows. <i>PNAS Nexus</i>. Oxford University
    Press. <a href="https://doi.org/10.1093/pnasnexus/pgag190">https://doi.org/10.1093/pnasnexus/pgag190</a>
  chicago: Stoev, Iliya D, Madison Bolger-Munro, Antonio Minopoli, Susan Wagner, Venkat
    Raghavan Krishnaswamy, Elena Erben, Kai Weißenbruch, et al. “Active and Probe-Free
    Intracellular Rheology via Phase-Sensitive Thermoviscous Flows.” <i>PNAS Nexus</i>.
    Oxford University Press, 2026. <a href="https://doi.org/10.1093/pnasnexus/pgag190">https://doi.org/10.1093/pnasnexus/pgag190</a>.
  ieee: I. D. Stoev <i>et al.</i>, “Active and probe-free intracellular rheology via
    phase-sensitive thermoviscous flows,” <i>PNAS Nexus</i>, vol. 5, no. 6. Oxford
    University Press, 2026.
  ista: Stoev ID, Bolger-Munro M, Minopoli A, Wagner S, Krishnaswamy VR, Erben E,
    Weißenbruch K, Maghelli N, Bastmeyer M, Heisenberg C-PJ, Kreysing M. 2026. Active
    and probe-free intracellular rheology via phase-sensitive thermoviscous flows.
    PNAS Nexus. 5(6), pgag190.
  mla: Stoev, Iliya D., et al. “Active and Probe-Free Intracellular Rheology via Phase-Sensitive
    Thermoviscous Flows.” <i>PNAS Nexus</i>, vol. 5, no. 6, pgag190, Oxford University
    Press, 2026, doi:<a href="https://doi.org/10.1093/pnasnexus/pgag190">10.1093/pnasnexus/pgag190</a>.
  short: I.D. Stoev, M. Bolger-Munro, A. Minopoli, S. Wagner, V.R. Krishnaswamy, E.
    Erben, K. Weißenbruch, N. Maghelli, M. Bastmeyer, C.-P.J. Heisenberg, M. Kreysing,
    PNAS Nexus 5 (2026).
das_tickbox: '1'
dataavailabilitystatement: 'All data and materials are made available on Zenodo public
  repository under Creative Commons Attribution 4.0 International License: https://doi.org/10.5281/zenodo.20322020.'
date_created: 2026-07-13T09:50:12Z
date_published: 2026-06-01T00:00:00Z
date_updated: 2026-07-13T13:14:43Z
day: '01'
ddc:
- '570'
department:
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doi: 10.1093/pnasnexus/pgag190
external_id:
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intvolume: '         5'
issue: '6'
keyword:
- cell mechanics
- active microrheology
- noninvasiveness
- thermoviscous flows
- FLUCS
language:
- iso: eng
month: '06'
oa: 1
oa_version: Published Version
publication: PNAS Nexus
publication_identifier:
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  - 2752-6542
publication_status: published
publisher: Oxford University Press
quality_controlled: '1'
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supplementarymaterial: yes
title: Active and probe-free intracellular rheology via phase-sensitive thermoviscous
  flows
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...
---
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abstract:
- lang: eng
  text: As seen in previous chapters, a graph game proceeds by placing a token on
    one of the vertices and allowing the players to move it throughout the graph to
    produce an infinite trace, which determines the winner or payoff of the game.
article_processing_charge: No
author:
- first_name: Guy
  full_name: Avni, Guy
  id: 463C8BC2-F248-11E8-B48F-1D18A9856A87
  last_name: Avni
  orcid: 0000-0001-5588-8287
- first_name: Thomas A
  full_name: Henzinger, Thomas A
  id: 40876CD8-F248-11E8-B48F-1D18A9856A87
  last_name: Henzinger
  orcid: 0000-0002-2985-7724
citation:
  ama: 'Avni G, Henzinger TA. Bidding Games. In: Fijalkow  ‪Nathanaël, ed. <i>Games
    on Graphs. From Logic and Automata to Algorithms</i>. Cambridge University Press;
    2026:529-569. doi:<a href="https://doi.org/10.1017/9781009500678.022">10.1017/9781009500678.022</a>'
  apa: Avni, G., &#38; Henzinger, T. A. (2026). Bidding Games. In  ‪Nathanaël Fijalkow
    (Ed.), <i>Games on Graphs. From Logic and Automata to Algorithms</i> (pp. 529–569).
    Cambridge University Press. <a href="https://doi.org/10.1017/9781009500678.022">https://doi.org/10.1017/9781009500678.022</a>
  chicago: Avni, Guy, and Thomas A Henzinger. “Bidding Games.” In <i>Games on Graphs.
    From Logic and Automata to Algorithms</i>, edited by  ‪Nathanaël Fijalkow, 529–69.
    Cambridge University Press, 2026. <a href="https://doi.org/10.1017/9781009500678.022">https://doi.org/10.1017/9781009500678.022</a>.
  ieee: G. Avni and T. A. Henzinger, “Bidding Games,” in <i>Games on Graphs. From
    Logic and Automata to Algorithms</i>,  ‪Nathanaël Fijalkow, Ed. Cambridge University
    Press, 2026, pp. 529–569.
  ista: 'Avni G, Henzinger TA. 2026.Bidding Games. In: Games on Graphs. From Logic
    and Automata to Algorithms. , 529–569.'
  mla: Avni, Guy, and Thomas A. Henzinger. “Bidding Games.” <i>Games on Graphs. From
    Logic and Automata to Algorithms</i>, edited by  ‪Nathanaël Fijalkow, Cambridge
    University Press, 2026, pp. 529–69, doi:<a href="https://doi.org/10.1017/9781009500678.022">10.1017/9781009500678.022</a>.
  short: G. Avni, T.A. Henzinger, in:,  ‪Nathanaël Fijalkow (Ed.), Games on Graphs.
    From Logic and Automata to Algorithms, Cambridge University Press, 2026, pp. 529–569.
corr_author: '1'
das_tickbox: '1'
date_created: 2026-07-13T10:44:22Z
date_published: 2026-04-26T00:00:00Z
date_updated: 2026-07-13T13:32:47Z
day: '26'
department:
- _id: ToHe
doi: 10.1017/9781009500678.022
editor:
- first_name: ' ‪Nathanaël'
  full_name: Fijalkow,  ‪Nathanaël
  last_name: Fijalkow
language:
- iso: eng
month: '04'
oa_version: None
page: 529-569
publication: Games on Graphs. From Logic and Automata to Algorithms
publication_identifier:
  eisbn:
  - '9781009500678'
  isbn:
  - '9781009500685'
publication_status: published
publisher: Cambridge University Press
quality_controlled: '1'
scopus_import: '1'
status: public
title: Bidding Games
type: book_chapter
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
year: '2026'
...
---
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abstract:
- lang: eng
  text: "We present the discovery of AT 2024wpp (‘Whippet’), a fast and luminous 18cow-like
    transient. At a redshift of z = 0 . 0868 , revealed by Keck Cosmic Web Imager
    spectroscopy of its faint star-forming host, it is the fourth-nearest example
    of its class to date. Rapid identification of the source in the Zwicky Transient
    Facility data stream permitted ultraviolet-through- optical observations to be
    obtained prior to peak, allowing the first determination of the peak bolometric
    luminosity ( 2 ×1045 erg s−1 ), maximum photospheric radius ( 1015 cm), and total
    radiated energy ( 1051 erg) of an 18cow-like object. We present results from a
    comprehensive multiwavelength observing campaign, including a far-ultraviolet
    spectrum from the Cosmic Origins Spectrograph on the Hubble Space Telescope and
    deep imaging extending > 100 d post-explosion from the Very Large Telescope, Hubble
    Space Telescope , Very Large Array, and Atacama Large Millimetre Array. We interpret
    the observations under a model in which a rapidly accreting central engine blows
    a fast ( ∼0.2 c ) wind into the surrounding medium and irradiates it with X-rays.
    The high Doppler velocities and intense ionization within this wind prevent identifiable
    spectroscopic features from appearing in the ejecta or in the surrounding circumstellar
    material. Weak H and He signatures do emerge in the spectra after 35 d in the
    form of double-peaked narrow lines. Each peak is individually narrow (full width
    δv ∼3000 km s−1 ) but the two components are separated by \x03v ∼6600 km s−1 ,
    indicating stable structures of denser material, possibly representing streams
    of tidal ejecta or an ablated companion star."
acknowledgement: "We thank Eliot Quataert, Luc Dessart, Ben Margalit, Ross Ferguson,
  Aaron Tohuvavohu, Brad Cenko, and Jamie Kennea for useful discussions. We thank
  the referee for helpful suggestions that improved the manuscript.\r\n\r\nBased on
  observations obtained with the Samuel Oschin Telescope 48-in. and the 60-in. Telescope
  at the Palomar Observatory as part of the Zwicky Transient Facility project. ZTF
  is supported by the National Science Foundation under grant no. AST-2034437 and
  a collaboration including Caltech, IPAC, the Oskar Klein Center at Stockholm University,
  the University of Maryland, University of California, Berkeley, the University of
  Wisconsin at Milwaukee, University of Warwick, Ruhr University Bochum, Cornell University,
  Northwestern University and Drexel University. Operations are conducted by COO,
  IPAC, and UW.\r\n\r\nThe Liverpool Telescope is operated on the island of La Palma
  by Liverpool John Moores University in the Spanish Observatorio del Roque de los
  Muchachos of the Instituto de Astrofisica de Canarias with financial support from
  the UK Science and Technology Facilities Council.\r\n\r\nBased on observations made
  with the Nordic Optical Telescope, owned in collaboration by the University of Turku
  and Aarhus University, and operated jointly by Aarhus University, the University
  of Turku and the University of Oslo, representing Denmark, Finland and Norway, the
  University of Iceland and Stockholm University at the Observatorio del Roque de
  los Muchachos, La Palma, Spain, of the Instituto de Astrofisica de Canarias. The
  NOT data were obtained under program ID 68–501.\r\n\r\nThis work made use of data
  supplied by the UK Swift Science Data Centre at the University of Leicester. We
  are grateful to Phil Evans, Aaron Tohuvavohu, and Jamie Kennea for advice on the
  Swift/XRT data reduction.\r\n\r\nSome of the data presented herein were obtained
  at the W. M. Keck Observatory, which is operated as a scientific partnership among
  the California Institute of Technology, the University of California, and NASA.
  The Observatory was made possible by the generous financial support of the W. M.
  Keck Foundation. The authors wish to recognize and acknowledge the very significant
  cultural role and reverence that the summit of Maunakea has always had within the
  indigenous Hawaiian community. We are most fortunate to have the opportunity to
  conduct observations from this mountain.\r\n\r\nSome observations reported here
  were obtained at the MMT Observatory, a joint facility of the University of Arizona
  and the Smithsonian Institution.\r\n\r\nThe National Radio Astronomy Observatory
  and Green Bank Observatory are facilities of the U.S. National Science Foundation
  operated under cooperative agreement by Associated Universities, Inc. This paper
  makes use of the following ALMA data: ADS/JAO.ALMA no. 2023.1.01730.T ALMA is a
  partnership of ESO (representing its member states), NSF (USA) and NINS (Japan),
  together with NRC (Canada), NSTC and ASIAA (Taiwan), and KASI (Republic of Korea),
  in cooperation with the Republic of Chile. The Joint ALMA Observatory is operated
  by ESO, AUI/NRAO, and NAOJ.\r\n\r\nBased on observations collected at the European
  Organisation for Astronomical Research in the Southern Hemisphere under ESO programme
  2114.D-5014(E). We thank John Pritchard and Paula Sanchez Saez, and the entire observatory
  staff, for their excellent support.\r\n\r\nBased on observations collected at the
  European Organisation for Astronomical Research in the Southern Hemisphere, Chile,
  as part of ePESSTO+ (the advanced Public ESO Spectroscopic Survey for Transient
  Objects Survey – PI: Inserra). ePESSTO+ observations were obtained under ESO program
  ID 112.25JQ.\r\n\r\nThis research is based on observations made with the NASA/ESA
  Hubble Space Telescope obtained from the Space Telescope Science Institute, which
  is operated by the Association of Universities for Research in Astronomy, Inc.,
  under NASA contract NAS 5–26555. These observations are associated with programs
  16714, 17477, and 17889.\r\n\r\nBased on observations obtained at the Southern Astrophysical
  Research (SOAR) telescope, which is a joint project of the Ministério da Ciência,
  Tecnologia e Inovações (MCTI/LNA) do Brasil, the US National Science Foundation’s
  NOIRLab, the University of North Carolina at Chapel Hill (UNC), and Michigan State
  University (MSU).\r\n\r\nThe Pan-STARRS1 Surveys (PS1) and the PS1 public science
  archive have been made possible through contributions by the Institute for Astronomy,
  the University of Hawaii, the Pan-STARRS Project Office, the Max-Planck Society
  and its participating institutes, the Max Planck Institute for Astronomy, Heidelberg
  and the Max Planck Institute for Extraterrestrial Physics, Garching, The Johns Hopkins
  University, Durham University, the University of Edinburgh, the Queen’s University
  Belfast, the Harvard-Smithsonian Center for Astrophysics, the Las Cumbres Observatory
  Global Telescope Network Incorporated, the National Central University of Taiwan,
  the Space Telescope Science Institute, the National Aeronautics and Space Administration
  under grant no. NNX08AR22G issued through the Planetary Science Division of the
  NASA Science Mission Directorate, the National Science Foundation grant no. AST–1238877,
  the University of Maryland, Eotvos Lorand University (ELTE), the Los Alamos National
  Laboratory, and the Gordon and Betty Moore Foundation.\r\n\r\nThis research made
  use of ccdproc, an astropy package for image reduction (M. Craig et al. 2025).\r\n\r\nGS
  and AYQH acknowledge support in part from a Sloan Research Fellowship (award no.
  FG-2024-21320) from the Alfred P. Sloan Foundation. CS and AYQH acknowledge support
  in part from National Aeronautics and Space Administration (NASA) grant 80NSSC24K0377,
  from HST grant HST-GO-17477.006-A, and from a Scialog award from the Research Corporation
  for Science Advancement (‘Early Science with the LSST’).\r\n\r\nPC acknowledges
  support from the Zhejiang Provincial Top-Level Research Support Program.\r\n\r\nIA
  and JC are supported by the National Science Foundation award AST 2505775, NASA
  grant 24-ADAP24-0159, Scialog award SA-LSST-2024-102a, and the Discovery Alliance
  Catalyst Fellowship Mentors award 2025-62192-CM-19\r\n\r\nAA acknowledges support
  from the Ministry of Education Yushan Fellow Program (MOE-111-YSFMS-0008-001-P1)
  and from the National Science and Technology Council, Taiwan (NSTC 114-2112-M-008-021-MY3).\r\n\r\nT-WC
  acknowledges support from the Ministry of Education Yushan Fellow Program (MOE-111-YSFMS-0008-001-P1)
  and from the National Science and Technology Council, Taiwan (NSTC 114-2112-M-008-021-MY3).\r\n\r\nERC
  acknowledges support from the National Aeronautics and Space Administration through
  the Astrophysics Theory Program, grant 80NSSC24K0897.\r\n\r\nGD acknowledges support
  from the European Union’s Horizon Europe research and innovation programme under
  the Marie Skłodowska-Curie grant agreement no. 101199369.\r\n\r\nDF’s contribution
  to this material is based upon work supported by the National Science Foundation
  under award no. AST-2401779.\r\n\r\nAGY’s research is supported by ISF, IMOS, and
  BSF grants, as well as the André Deloro Institute for Space and Optics Research,
  the Center for Experimental Physics, a WIS-MIT Sagol grant, the Norman E Alexander
  Family M Foundation ULTRASAT Data Center Fund, and Yeda-Sela; AGY is the incumbent
  of the The Arlyn Imberman Professorial Chair.\r\n\r\nLG acknowledges financial support
  from AGAUR, CSIC, MCIN, and AEI 10.13039/501100011033 under projects PID2023-151307NB-I00,
  PIE 20215AT016, and CEX2020-001058-M.\r\n\r\nMG acknowledges support from an STFC
  PhD studentship and from the Faculty of Science and Technology at Lancaster University.\r\n\r\nCPG
  acknowledges financial support from the Secretary of Universities and Research (Government
  of Catalonia) and by the Horizon 2020 Research and Innovation Programme of the European
  Union under the Marie Skłodowska-Curie and the Beatriu de Pinós 2021 BP 00168 programme,
  from the Spanish Ministerio de Ciencia e Innovación (MCIN) and the Agencia Estatal
  de Investigación (AEI) 10.13039/501100011033 under the PID2023-151307NB-I00 SNNEXT
  project, from Centro Superior de Investigaciones Científicas (CSIC) under the PIE
  project 20215AT016 and the program Unidad de Excelencia María de Maeztu CEX2020-001058-M,
  and from the Departament de Recerca i Universitats de la Generalitat de Catalunya
  through the 2021-SGR-01270 grant.\r\n\r\nCL is supported by DoE award no.  DE-SC0025599.\r\n\r\nZwicky
  Transient Facility, W. M. Keck Observatory, and MMT Observatory access was supported
  by Northwestern University and the Center for Interdisciplinary Exploration and
  Research in Astrophysics (CIERA).\r\n\r\nAM gratefully acknowledges support from
  an STFC PhD studentship and the Faculty of Science and Technology at Lancaster University.\r\n\r\nTEMB
  is funded by Horizon Europe ERC grant no. 101125877.\r\n\r\nMN is supported by the
  European Research Council (ERC) under the European Union’s Horizon 2020 research
  and innovation programme (grant agreement no. 948381).\r\n\r\nNR is supported by
  a Northwestern University Presidential Fellowship Award. We gratefully acknowledge
  the support of the NSF-Simons AI-Institute for the Sky (SkAI) via grants NSF AST-2421845
  and Simons Foundation MPS-AI-00010513.\r\n\r\nAS acknowledges the Warwick Astrophysics
  PhD prize scholarship made possible thanks to a generous philanthropic donation.\r\n\r\nSJS
  acknowledges funding from STFC grant ST/Y001605/1, a Royal Society Research Professorship
  and the Hintze Family Charitable Foundation."
article_number: stag678
article_processing_charge: Yes
article_type: original
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  full_name: Perley, Daniel A
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  full_name: Govreen-Segal, Taya
  last_name: Govreen-Segal
- first_name: Aleksandra
  full_name: Bochenek, Aleksandra
  last_name: Bochenek
- first_name: Yu-Jing
  full_name: Qin, Yu-Jing
  last_name: Qin
- first_name: James H
  full_name: Gillanders, James H
  last_name: Gillanders
- first_name: Benjamin
  full_name: Amend, Benjamin
  last_name: Amend
- first_name: Joseph P
  full_name: Anderson, Joseph P
  last_name: Anderson
- first_name: Igor
  full_name: Andreoni, Igor
  last_name: Andreoni
- first_name: Amar
  full_name: Aryan, Amar
  last_name: Aryan
- first_name: Eric C
  full_name: Bellm, Eric C
  last_name: Bellm
- first_name: Joshua S
  full_name: Bloom, Joshua S
  last_name: Bloom
- first_name: Thomas
  full_name: de Boer, Thomas
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- first_name: Jonathan
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  orcid: 0000-0002-4770-5388
- first_name: Ken C
  full_name: Chambers, Ken C
  last_name: Chambers
- first_name: Panos
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  last_name: Charalampopoulos
- first_name: Ting-Wan
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- first_name: Tracy X
  full_name: Chen, Tracy X
  last_name: Chen
- first_name: Eric R
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- first_name: Matthew J
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- first_name: Steven L
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- first_name: Claudia P
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- first_name: K -Ryan
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- first_name: Mark E
  full_name: Huber, Mark E
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- first_name: Cosimo
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- first_name: Benjamin C
  full_name: Kaiser, Benjamin C
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- first_name: Mansi M
  full_name: Kasliwal, Mansi M
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- first_name: Niilo E
  full_name: Koivisto, Niilo E
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- first_name: Chien-Cheng
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- first_name: Chang
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- first_name: Thomas B
  full_name: Lowe, Thomas B
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  last_name: Magnier
- first_name: Ashish A
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- first_name: Tomás E
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  last_name: Müller-Bravo
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- first_name: Priscila J
  full_name: Pessi, Priscila J
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  full_name: Sahu, Anwesha
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  full_name: Singh, Avinash
  last_name: Singh
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  full_name: Smith, Ian A
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  full_name: Sollerman, Jesper
  last_name: Sollerman
- first_name: Gokul
  full_name: Srinivasaragavan, Gokul
  last_name: Srinivasaragavan
- first_name: Shubham
  full_name: Srivastav, Shubham
  last_name: Srivastav
- first_name: Robert D
  full_name: Stein, Robert D
  last_name: Stein
- first_name: Steve
  full_name: Schulze, Steve
  last_name: Schulze
- first_name: Jack W
  full_name: Tweddle, Jack W
  last_name: Tweddle
- first_name: Richard
  full_name: Wainscoat, Richard
  last_name: Wainscoat
- first_name: Jacob L
  full_name: Wise, Jacob L
  last_name: Wise
- first_name: Lin
  full_name: Yan, Lin
  last_name: Yan
- first_name: David R
  full_name: Young, David R
  last_name: Young
citation:
  ama: 'Perley DA, Ho AYQ, McGrath Z, et al. AT 2024wpp: An extremely luminous fast
    ultraviolet transient powered by accretion onto a black hole. <i>Monthly Notices
    of the Royal Astronomical Society</i>. 2026;549(1). doi:<a href="https://doi.org/10.1093/mnras/stag678">10.1093/mnras/stag678</a>'
  apa: 'Perley, D. A., Ho, A. Y. Q., McGrath, Z., Camilo, M., Sevilla, C., Chen, P.,
    … Young, D. R. (2026). AT 2024wpp: An extremely luminous fast ultraviolet transient
    powered by accretion onto a black hole. <i>Monthly Notices of the Royal Astronomical
    Society</i>. Oxford University Press. <a href="https://doi.org/10.1093/mnras/stag678">https://doi.org/10.1093/mnras/stag678</a>'
  chicago: 'Perley, Daniel A, Anna Y Q Ho, Zoë McGrath, Michael Camilo, Cassie Sevilla,
    Ping Chen, Genevieve Schroeder, et al. “AT 2024wpp: An Extremely Luminous Fast
    Ultraviolet Transient Powered by Accretion onto a Black Hole.” <i>Monthly Notices
    of the Royal Astronomical Society</i>. Oxford University Press, 2026. <a href="https://doi.org/10.1093/mnras/stag678">https://doi.org/10.1093/mnras/stag678</a>.'
  ieee: 'D. A. Perley <i>et al.</i>, “AT 2024wpp: An extremely luminous fast ultraviolet
    transient powered by accretion onto a black hole,” <i>Monthly Notices of the Royal
    Astronomical Society</i>, vol. 549, no. 1. Oxford University Press, 2026.'
  ista: 'Perley DA, Ho AYQ, McGrath Z, Camilo M, Sevilla C, Chen P, Schroeder G, Govreen-Segal
    T, Bochenek A, Qin Y-J, Gillanders JH, Amend B, Anderson JP, Andreoni I, Aryan
    A, Bellm EC, Bloom JS, de Boer T, Carney J, Caiazzo I, Chambers KC, Charalampopoulos
    P, Chen T-W, Chen TX, Coughlin ER, Coughlin M, Dennefeld M, Dimitriadis G, Fremling
    C, Frostig D, Gal-Yam A, Galbany L, Gangopadhyay A, Ghendrih M, Graham MJ, Gromadzki
    M, Groom SL, Gutiérrez CP, Hinds K-R, Huber ME, Inserra C, Kaiser BC, Kasliwal
    MM, Koivisto NE, Lin C-C, Liu C, Lowe TB, Magnier E, Mahabal AA, Milligan A, Minguez
    P, Mo G, Müller-Bravo TE, Nicholl M, Pessi PJ, Pignata G, Purdum J, Rehemtulla
    N, Rich RM, Sahu A, Singh A, Smartt SJ, Smith IA, Sollerman J, Srinivasaragavan
    G, Srivastav S, Stein RD, Schulze S, Tweddle JW, Wainscoat R, Wise JL, Yan L,
    Young DR. 2026. AT 2024wpp: An extremely luminous fast ultraviolet transient powered
    by accretion onto a black hole. Monthly Notices of the Royal Astronomical Society.
    549(1), stag678.'
  mla: 'Perley, Daniel A., et al. “AT 2024wpp: An Extremely Luminous Fast Ultraviolet
    Transient Powered by Accretion onto a Black Hole.” <i>Monthly Notices of the Royal
    Astronomical Society</i>, vol. 549, no. 1, stag678, Oxford University Press, 2026,
    doi:<a href="https://doi.org/10.1093/mnras/stag678">10.1093/mnras/stag678</a>.'
  short: D.A. Perley, A.Y.Q. Ho, Z. McGrath, M. Camilo, C. Sevilla, P. Chen, G. Schroeder,
    T. Govreen-Segal, A. Bochenek, Y.-J. Qin, J.H. Gillanders, B. Amend, J.P. Anderson,
    I. Andreoni, A. Aryan, E.C. Bellm, J.S. Bloom, T. de Boer, J. Carney, I. Caiazzo,
    K.C. Chambers, P. Charalampopoulos, T.-W. Chen, T.X. Chen, E.R. Coughlin, M. Coughlin,
    M. Dennefeld, G. Dimitriadis, C. Fremling, D. Frostig, A. Gal-Yam, L. Galbany,
    A. Gangopadhyay, M. Ghendrih, M.J. Graham, M. Gromadzki, S.L. Groom, C.P. Gutiérrez,
    K.-R. Hinds, M.E. Huber, C. Inserra, B.C. Kaiser, M.M. Kasliwal, N.E. Koivisto,
    C.-C. Lin, C. Liu, T.B. Lowe, E. Magnier, A.A. Mahabal, A. Milligan, P. Minguez,
    G. Mo, T.E. Müller-Bravo, M. Nicholl, P.J. Pessi, G. Pignata, J. Purdum, N. Rehemtulla,
    R.M. Rich, A. Sahu, A. Singh, S.J. Smartt, I.A. Smith, J. Sollerman, G. Srinivasaragavan,
    S. Srivastav, R.D. Stein, S. Schulze, J.W. Tweddle, R. Wainscoat, J.L. Wise, L.
    Yan, D.R. Young, Monthly Notices of the Royal Astronomical Society 549 (2026).
das_tickbox: '1'
dataavailabilitystatement: All photometry is provided in the supplementary data files.
  Spectroscopy will be made available on WISEREP, and is available on request to the
  lead author.
date_created: 2026-07-13T10:50:10Z
date_published: 2026-06-01T00:00:00Z
date_updated: 2026-07-13T14:36:24Z
day: '01'
ddc:
- '520'
department:
- _id: IlCa
doi: 10.1093/mnras/stag678
external_id:
  arxiv:
  - '2601.03337'
file:
- access_level: open_access
  checksum: a5827b9f68f1731b8c8df18142c0ef38
  content_type: application/pdf
  creator: dernst
  date_created: 2026-07-13T14:35:34Z
  date_updated: 2026-07-13T14:35:34Z
  file_id: '22314'
  file_name: 2026_MNRAS_Perley.pdf
  file_size: 6208809
  relation: main_file
  success: 1
file_date_updated: 2026-07-13T14:35:34Z
has_accepted_license: '1'
intvolume: '       549'
issue: '1'
keyword:
- 'stars: black holes'
- 'supernovae: individual: AT2024wpp'
- 'radio continuum: transients'
language:
- iso: eng
month: '06'
oa: 1
oa_version: Published Version
publication: Monthly Notices of the Royal Astronomical Society
publication_identifier:
  eissn:
  - 1365-2966
  issn:
  - 0035-8711
publication_status: published
publisher: Oxford University Press
quality_controlled: '1'
researchdata_availability: upon request
scopus_import: '1'
status: public
supplementarymaterial: yes
title: 'AT 2024wpp: An extremely luminous fast ultraviolet transient powered by accretion
  onto a black hole'
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 549
year: '2026'
...
---
OA_place: publisher
OA_type: hybrid
PlanS_conform: '1'
_id: '22301'
abstract:
- lang: eng
  text: Auxin, primarily indole-3-acetic acid (IAA), is a central regulator of growth
    and development in land plants, but its physiological role in chlorophyte algae
    remains unclear. Here, we show that exogenous IAA modulates growth in Chlorella
    sorokiniana, Chlorella variabilis, and Chlamydomonas reinhardtii in a concentration-dependent
    manner. Low IAA concentrations promoted growth by accelerating the onset of cell
    division without affecting cell size, whereas higher concentrations inhibited
    proliferation. Radiotracer assays showed that all three species take up and release
    IAA across the plasma membrane through a combination of passive diffusion and
    energy-dependent, saturable processes. Competition by excess unlabeled natural
    and synthetic auxins further supported the presence of carrier-mediated transport
    with broad substrate recognition. Phylogenetic analyses identified potential PIN-like
    auxin exporters in chlorophytes and other non-plant eukaryotes, and structural
    modeling supported conservation of the overall PIN fold and predicted auxin-binding
    residues. However, functional assays in Xenopus laevis oocytes, tobacco BY-2 cultured
    cells, and Arabidopsis thaliana did not support a role for these proteins in directional
    auxin export. Instead, non-plant PIN homologs localized predominantly to the endoplasmic
    reticulum and showed limited or no transport activity in heterologous systems.
    Together, these findings indicate that auxin responsiveness and basic cellular
    auxin transport predate canonical PIN-mediated directional auxin export, which
    appears to be a later innovation of the streptophyte lineage.
acknowledged_ssus:
- _id: Bio
- _id: NanoFab
acknowledgement: Research in the Friml group was supported by the European Research
  Council (ERC) under grant agreement No. 101142681 (CYNIPS), and by the Austrian
  Science Fund (FWF) through projects I 6123-B and P 37051-B. A DOC Fellowship from
  the Austrian Academy of Sciences (ÖAW; PR.C0102.1.F.1023.A.2) provided additional
  support. Work was partly supported by the Deutsche Forschungsgemeinschaft (DFG,
  German Research Foundation) under grant HA 3468/8-1. We thank the Imaging and Optics
  Facility (IOF) at the Institute of Science and Technology Austria (ISTA) for support
  with confocal imaging, and the Nanofabrication Facility at ISTA for assistance with
  microfluidic device fabrication. We also acknowledge the microscopy service of IFIEB
  CAS, supported by MEYS CR (LM2023050 Czech-BioImaging). Open Access funding provided
  by Institute of Science and Technology Austria.
article_number: jipb.70309
article_processing_charge: Yes (via OA deal)
article_type: original
author:
- first_name: Adrijana
  full_name: Smoljan, Adrijana
  id: cced8a85-223e-11ed-af04-b0596c55053b
  last_name: Smoljan
- first_name: Sarah
  full_name: Koutnik‐Abele, Sarah
  last_name: Koutnik‐Abele
- first_name: Dmitrii
  full_name: Vladimirtsev, Dmitrii
  id: 60466724-5355-11ee-ae5a-fa55e8f99c3d
  last_name: Vladimirtsev
- first_name: Petr
  full_name: Klíma, Petr
  last_name: Klíma
- first_name: Anita
  full_name: Bírošíková, Anita
  last_name: Bírošíková
- first_name: Yuzhou
  full_name: Zhang, Yuzhou
  id: 3B6137F2-F248-11E8-B48F-1D18A9856A87
  last_name: Zhang
  orcid: 0000-0003-2627-6956
- first_name: Jack
  full_name: Merrin, Jack
  id: 4515C308-F248-11E8-B48F-1D18A9856A87
  last_name: Merrin
  orcid: 0000-0001-5145-4609
- first_name: Maximilian
  full_name: Schuster, Maximilian
  id: 37e65def-d415-11eb-ae59-a7b67be103db
  last_name: Schuster
- first_name: Katarina
  full_name: Kurtović, Katarina
  last_name: Kurtović
- first_name: Ulrich Z.
  full_name: Hammes, Ulrich Z.
  last_name: Hammes
- first_name: Jan
  full_name: Petrášek, Jan
  last_name: Petrášek
- first_name: Jiří
  full_name: Friml, Jiří
  id: 4159519E-F248-11E8-B48F-1D18A9856A87
  last_name: Friml
  orcid: 0000-0002-8302-7596
citation:
  ama: Smoljan A, Koutnik‐Abele S, Vladimirtsev D, et al. Auxin response and PIN‐mediated
    transport in chlorophyte algae. <i>Journal of Integrative Plant Biology</i>. 2026.
    doi:<a href="https://doi.org/10.1111/jipb.70309">10.1111/jipb.70309</a>
  apa: Smoljan, A., Koutnik‐Abele, S., Vladimirtsev, D., Klíma, P., Bírošíková, A.,
    Zhang, Y., … Friml, J. (2026). Auxin response and PIN‐mediated transport in chlorophyte
    algae. <i>Journal of Integrative Plant Biology</i>. Wiley. <a href="https://doi.org/10.1111/jipb.70309">https://doi.org/10.1111/jipb.70309</a>
  chicago: Smoljan, Adrijana, Sarah Koutnik‐Abele, Dmitrii Vladimirtsev, Petr Klíma,
    Anita Bírošíková, Yuzhou Zhang, Jack Merrin, et al. “Auxin Response and PIN‐mediated
    Transport in Chlorophyte Algae.” <i>Journal of Integrative Plant Biology</i>.
    Wiley, 2026. <a href="https://doi.org/10.1111/jipb.70309">https://doi.org/10.1111/jipb.70309</a>.
  ieee: A. Smoljan <i>et al.</i>, “Auxin response and PIN‐mediated transport in chlorophyte
    algae,” <i>Journal of Integrative Plant Biology</i>. Wiley, 2026.
  ista: Smoljan A, Koutnik‐Abele S, Vladimirtsev D, Klíma P, Bírošíková A, Zhang Y,
    Merrin J, Schuster M, Kurtović K, Hammes UZ, Petrášek J, Friml J. 2026. Auxin
    response and PIN‐mediated transport in chlorophyte algae. Journal of Integrative
    Plant Biology., jipb. 70309.
  mla: Smoljan, Adrijana, et al. “Auxin Response and PIN‐mediated Transport in Chlorophyte
    Algae.” <i>Journal of Integrative Plant Biology</i>, jipb. 70309, Wiley, 2026,
    doi:<a href="https://doi.org/10.1111/jipb.70309">10.1111/jipb.70309</a>.
  short: A. Smoljan, S. Koutnik‐Abele, D. Vladimirtsev, P. Klíma, A. Bírošíková, Y.
    Zhang, J. Merrin, M. Schuster, K. Kurtović, U.Z. Hammes, J. Petrášek, J. Friml,
    Journal of Integrative Plant Biology (2026).
corr_author: '1'
das_tickbox: '0'
date_created: 2026-07-13T10:44:55Z
date_published: 2026-06-10T00:00:00Z
date_updated: 2026-07-13T14:26:31Z
day: '10'
ddc:
- '580'
department:
- _id: JiFr
- _id: GradSch
- _id: NanoFab
- _id: Bio
doi: 10.1111/jipb.70309
external_id:
  pmid:
  - '42271607'
has_accepted_license: '1'
language:
- iso: eng
main_file_link:
- open_access: '1'
  url: https://doi.org/10.1111/jipb.70309
month: '06'
oa: 1
oa_version: Published Version
pmid: 1
project:
- _id: 8f347782-16d5-11f0-9cad-8c19706ee739
  grant_number: '101142681'
  name: Cyclic nucleotides as second messengers in plants
- _id: bd76d395-d553-11ed-ba76-f678c14f9033
  grant_number: I06123
  name: Peptide receptors for auxin canalization in Arabidopsis
- _id: 7bcece63-9f16-11ee-852c-ae94e099eeb6
  grant_number: P37051
  name: Guanylate cyclase activity of TIR1/AFBs auxin receptors
publication: Journal of Integrative Plant Biology
publication_identifier:
  eissn:
  - 1744-7909
  issn:
  - 1672-9072
publication_status: epub_ahead
publisher: Wiley
quality_controlled: '1'
researchdata_availability: no
scopus_import: '1'
status: public
supplementarymaterial: yes
title: Auxin response and PIN‐mediated transport in chlorophyte algae
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
year: '2026'
...
---
OA_place: publisher
OA_type: hybrid
_id: '22129'
abstract:
- lang: eng
  text: "Inside–outside classification is widely used for geometry processing tasks
    such as surface reconstruction, geometry completion,\r\nand calculating signed
    distance fields. We introduce a new integral formulation of this problem, which
    assigns confidence\r\nscores that points are inside or outside, given incomplete
    boundary geometry. Even though our geometric construction does\r\nnot appear in
    previous work, we show that it is unexpectedly linked to both the well-established
    generalized winding number\r\n(GWN) and pseudonormal methods for geometry completion,
    and it provably reduces to either one of them for specific values\r\nof a control
    parameter. The results obtained with our method frequently outperform screened
    Poisson surface reconstruction\r\n(PSR), GWN, and the pseudonormal method in terms
    of quality, and are at least on par with them on all of our examples. Unlike\r\nthese
    methods, our algorithm naturally extends to the multi-label setting, in which
    regions with an arbitrary number of colors\r\nor physical materials can be reconstructed,
    and non-manifold features such as T-junctions may appear in the interface and\r\nboundary
    geometry"
article_processing_charge: Yes (via OA deal)
author:
- first_name: 'Ziyu '
  full_name: 'Wei, Ziyu '
  last_name: Wei
- first_name: Christian
  full_name: Hafner, Christian
  id: 400429CC-F248-11E8-B48F-1D18A9856A87
  last_name: Hafner
- first_name: Aleksei
  full_name: Kalinov, Aleksei
  id: 44b7120e-eb97-11eb-a6c2-e1557aa81d02
  last_name: Kalinov
  orcid: 0000-0003-2189-3904
- first_name: Peter
  full_name: Synak, Peter
  id: 331776E2-F248-11E8-B48F-1D18A9856A87
  last_name: Synak
- first_name: Christopher J
  full_name: Wojtan, Christopher J
  id: 3C61F1D2-F248-11E8-B48F-1D18A9856A87
  last_name: Wojtan
  orcid: 0000-0001-6646-5546
citation:
  ama: 'Wei Z, Hafner C, Kalinov A, Synak P, Wojtan C. Circles of confidence for multi-label
    geometry completion. In: <i>Computer Graphics Forum</i>. Vol 45. Wiley. doi:<a
    href="https://doi.org/10.1111/cgf.70516">10.1111/cgf.70516</a>'
  apa: 'Wei, Z., Hafner, C., Kalinov, A., Synak, P., &#38; Wojtan, C. (n.d.). Circles
    of confidence for multi-label geometry completion. In <i>Computer Graphics Forum</i>
    (Vol. 45). Bern, Switzerland: Wiley. <a href="https://doi.org/10.1111/cgf.70516">https://doi.org/10.1111/cgf.70516</a>'
  chicago: Wei, Ziyu , Christian Hafner, Aleksei Kalinov, Peter Synak, and Chris Wojtan.
    “Circles of Confidence for Multi-Label Geometry Completion.” In <i>Computer Graphics
    Forum</i>, Vol. 45. Wiley, n.d. <a href="https://doi.org/10.1111/cgf.70516">https://doi.org/10.1111/cgf.70516</a>.
  ieee: Z. Wei, C. Hafner, A. Kalinov, P. Synak, and C. Wojtan, “Circles of confidence
    for multi-label geometry completion,” in <i>Computer Graphics Forum</i>, Bern,
    Switzerland, vol. 45, no. 5.
  ista: 'Wei Z, Hafner C, Kalinov A, Synak P, Wojtan C. Circles of confidence for
    multi-label geometry completion. Computer Graphics Forum. Eurographics: Symposium
    on Geometry Processing vol. 45.'
  mla: Wei, Ziyu, et al. “Circles of Confidence for Multi-Label Geometry Completion.”
    <i>Computer Graphics Forum</i>, vol. 45, no. 5, Wiley, doi:<a href="https://doi.org/10.1111/cgf.70516">10.1111/cgf.70516</a>.
  short: Z. Wei, C. Hafner, A. Kalinov, P. Synak, C. Wojtan, in:, Computer Graphics
    Forum, Wiley, n.d.
conference:
  end_date: 2026-07-03
  location: Bern, Switzerland
  name: 'Eurographics: Symposium on Geometry Processing'
  start_date: 2026-07-01
corr_author: '1'
das_tickbox: '1'
date_created: 2026-06-23T09:08:41Z
date_published: 2026-06-24T00:00:00Z
date_updated: 2026-07-13T14:58:48Z
day: '24'
ddc:
- '005'
department:
- _id: ChWo
- _id: GradSch
doi: 10.1111/cgf.70516
file:
- access_level: open_access
  checksum: 365f986db34e3fbce74089207599253b
  content_type: application/pdf
  creator: mly
  date_created: 2026-06-23T09:07:22Z
  date_updated: 2026-06-23T09:07:22Z
  file_id: '22132'
  file_name: document(3).pdf
  file_size: 14536575
  relation: main_file
  success: 1
file_date_updated: 2026-06-23T09:07:22Z
has_accepted_license: '1'
intvolume: '        45'
issue: '5'
language:
- iso: eng
month: '06'
oa: 1
oa_version: Published Version
project:
- _id: 34bc2376-11ca-11ed-8bc3-9a3b3961a088
  grant_number: '101045083'
  name: Computational Discovery of Numerical Algorithms for Animation and Simulation
    of Natural Phenomena
publication: Computer Graphics Forum
publication_status: accepted
publisher: Wiley
quality_controlled: '1'
status: public
title: Circles of confidence for multi-label geometry completion
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: conference
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 45
year: '2026'
...
---
OA_place: publisher
OA_type: gold
_id: '22299'
abstract:
- lang: eng
  text: The depth poset of a filtered Lefschetz complex reflects the dependencies
    between the cancellations of different shallow birth-death pairs. Using the fast
    algorithms for computing the depth poset in [Edelsbrunner et al., 2026] and for
    updating the persistence diagram under transpositions in [Cohen-Steiner et al.,
    2006], we give a complete case analysis of how transpositions of cells in the
    filter affect the depth poset. In addition, we present statistics on the depth
    poset for random point data and its sensitivity to the transpositions that occur
    in random straight-line homotopies.
acknowledgement: "The authors thank Jakub Leśkiewicz and Bartosz Furmanek for discussions\r\nthat
  helped improve the paper. Herbert Edelsbrunner: DFG Collaborative Research Center
  TRR 109, Austrian Science\r\nFund (FWF), grant no. I 02979-N35\r\nMichał Lipiński:
  European Union’s Horizon 2020 research and innovation programme under the\r\nMarie
  Skłodowska-Curie Grant Agreement No. 101034413\r\nMarian Mrozek: Polish National
  Science Center under Opus Grant 2019/35/B/ST1/00874 and Opus\r\nGrant 2025/57/B/ST1/00550"
alternative_title:
- LIPIcs
article_number: 41:1-41:18
article_processing_charge: Yes
arxiv: 1
author:
- first_name: Herbert
  full_name: Edelsbrunner, Herbert
  id: 3FB178DA-F248-11E8-B48F-1D18A9856A87
  last_name: Edelsbrunner
  orcid: 0000-0002-9823-6833
- first_name: Michał
  full_name: Lipiński, Michał
  id: dfffb474-4317-11ee-8f5c-fe3fc95a425e
  last_name: Lipiński
  orcid: 0000-0001-9789-9750
- first_name: Marian
  full_name: Mrozek, Marian
  last_name: Mrozek
  orcid: 0000-0002-0619-6417
- first_name: Manuel
  full_name: Soriano Trigueros, Manuel
  id: 15ebd7cf-15bf-11ee-aebd-bb4bb5121ea8
  last_name: Soriano Trigueros
  orcid: 0000-0003-2449-1433
- first_name: Fedor
  full_name: Zimin, Fedor
  id: afd27eda-91c1-11f0-aad8-c6edbec24c04
  last_name: Zimin
citation:
  ama: 'Edelsbrunner H, Lipiński M, Mrozek M, Soriano Trigueros M, Zimin F. The depth
    poset under transpositions in the filter. In: <i>42nd International Symposium
    on Computational Geometry</i>. Vol 367. Schloss Dagstuhl – Leibniz-Zentrum für
    Informatik; 2026. doi:<a href="https://doi.org/10.4230/LIPICS.SOCG.2026.41">10.4230/LIPICS.SOCG.2026.41</a>'
  apa: 'Edelsbrunner, H., Lipiński, M., Mrozek, M., Soriano Trigueros, M., &#38; Zimin,
    F. (2026). The depth poset under transpositions in the filter. In <i>42nd International
    Symposium on Computational Geometry</i> (Vol. 367). New Brunswick, NJ, United
    States: Schloss Dagstuhl – Leibniz-Zentrum für Informatik. <a href="https://doi.org/10.4230/LIPICS.SOCG.2026.41">https://doi.org/10.4230/LIPICS.SOCG.2026.41</a>'
  chicago: Edelsbrunner, Herbert, Michał Lipiński, Marian Mrozek, Manuel Soriano Trigueros,
    and Fedor Zimin. “The Depth Poset under Transpositions in the Filter.” In <i>42nd
    International Symposium on Computational Geometry</i>, Vol. 367. Schloss Dagstuhl
    – Leibniz-Zentrum für Informatik, 2026. <a href="https://doi.org/10.4230/LIPICS.SOCG.2026.41">https://doi.org/10.4230/LIPICS.SOCG.2026.41</a>.
  ieee: H. Edelsbrunner, M. Lipiński, M. Mrozek, M. Soriano Trigueros, and F. Zimin,
    “The depth poset under transpositions in the filter,” in <i>42nd International
    Symposium on Computational Geometry</i>, New Brunswick, NJ, United States, 2026,
    vol. 367.
  ista: 'Edelsbrunner H, Lipiński M, Mrozek M, Soriano Trigueros M, Zimin F. 2026.
    The depth poset under transpositions in the filter. 42nd International Symposium
    on Computational Geometry. SoCG: Symposium on Computational Geometry, LIPIcs,
    vol. 367, 41:1-41:18.'
  mla: Edelsbrunner, Herbert, et al. “The Depth Poset under Transpositions in the
    Filter.” <i>42nd International Symposium on Computational Geometry</i>, vol. 367,
    41:1-41:18, Schloss Dagstuhl – Leibniz-Zentrum für Informatik, 2026, doi:<a href="https://doi.org/10.4230/LIPICS.SOCG.2026.41">10.4230/LIPICS.SOCG.2026.41</a>.
  short: H. Edelsbrunner, M. Lipiński, M. Mrozek, M. Soriano Trigueros, F. Zimin,
    in:, 42nd International Symposium on Computational Geometry, Schloss Dagstuhl
    – Leibniz-Zentrum für Informatik, 2026.
conference:
  end_date: 2026-06-05
  location: New Brunswick, NJ, United States
  name: 'SoCG: Symposium on Computational Geometry'
  start_date: 2026-06-02
corr_author: '1'
das_tickbox: '0'
date_created: 2026-07-13T09:56:38Z
date_published: 2026-05-27T00:00:00Z
date_updated: 2026-07-14T06:09:32Z
day: '27'
ddc:
- '500'
department:
- _id: HeEd
- _id: GradSch
doi: 10.4230/LIPICS.SOCG.2026.41
ec_funded: 1
external_id:
  arxiv:
  - '2511.21961'
file:
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  relation: main_file
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file_date_updated: 2026-07-14T06:08:05Z
has_accepted_license: '1'
intvolume: '       367'
keyword:
- Algebraic topology
- Lefschetz complexes
- persistent homology
- vines and vineyards
- birth-death pairs
- shallow pairs
- relations
- partial orders
- transpositions
- Theory of computation → Computational geometry
language:
- iso: eng
month: '05'
oa: 1
oa_version: Published Version
project:
- _id: 2561EBF4-B435-11E9-9278-68D0E5697425
  call_identifier: FWF
  grant_number: I02979-N35
  name: Persistence and stability of geometric complexes
- _id: fc2ed2f7-9c52-11eb-aca3-c01059dda49c
  call_identifier: H2020
  grant_number: '101034413'
  name: 'IST-BRIDGE: International postdoctoral program'
publication: 42nd International Symposium on Computational Geometry
publication_identifier:
  eissn:
  - 1868-8969
  isbn:
  - '9783959774185'
publication_status: published
publisher: Schloss Dagstuhl – Leibniz-Zentrum für Informatik
quality_controlled: '1'
researchdata_availability: no
scopus_import: '1'
status: public
supplementarymaterial: no
title: The depth poset under transpositions in the filter
tmp:
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...
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OA_type: gold
_id: '22298'
abstract:
- lang: eng
  text: Air traffic management is a critical component of aviation, aiming to balance
    safety, capacity and demand within controlled airspace. This research analyses
    Iran's domestic air transport network (2018-2021) by developing annual Origin-Destination
    (OD) impedance matrices based on flight frequency. The methodology quantifies
    network connectivity, revealing a highly centralized structure dominated by core
    corridors like Tehran-Mashhad, which carried over 10,500 flights in 2019. The
    COVID-19 pandemic caused a severe disruption in 2020, with traffic on major routes
    falling by nearly half, followed by a partial recovery in 2021. Analysis shows
    core hubs rebounded faster than peripheral airports, widening accessibility gaps.
    Through origin-destination matrix processing, the system identifies high density
    air routes and analyses historical trends in airspace utilization. The impedance
    matrix, validated against data (R²=0.87), successfully maps the intense service
    on hub links and the high impedance of sparse peripheral routes. Then an interactive
    Web GIS platform was implemented for spatiotemporal analysis of air traffic density.
acknowledgement: "We sincerely thank the Iranian Airports and Air Navigation\r\nCompany
  for sharing statistical data on flights from Iranian\r\nairports, separated by origin
  and destination, for this research."
article_processing_charge: No
author:
- first_name: Masoumeh
  full_name: Eghbali Mardekheh, Masoumeh
  last_name: Eghbali Mardekheh
- first_name: Meysam
  full_name: Argany, Meysam
  last_name: Argany
- first_name: Farid
  full_name: Karimipour, Farid
  id: 2A2BCDC4-CF62-11E9-BE5E-3B1EE6697425
  last_name: Karimipour
  orcid: 0000-0001-6746-4174
- first_name: Seyed Mohammad
  full_name: Sedghitabar, Seyed Mohammad
  last_name: Sedghitabar
citation:
  ama: 'Eghbali Mardekheh M, Argany M, Karimipour F, Sedghitabar SM. Real time interactive
    web GIS based modelling of high traffic air corridors in Iran using origin destination
    matrix analysis. In: <i>8th ISPRS Geospatial Conference</i>. Vol X. Copernicus
    Publications; 2026:493-500. doi:<a href="https://doi.org/10.5194/isprs-annals-x-4-w8-2025-493-2026">10.5194/isprs-annals-x-4-w8-2025-493-2026</a>'
  apa: 'Eghbali Mardekheh, M., Argany, M., Karimipour, F., &#38; Sedghitabar, S. M.
    (2026). Real time interactive web GIS based modelling of high traffic air corridors
    in Iran using origin destination matrix analysis. In <i>8th ISPRS Geospatial Conference</i>
    (Vol. X, pp. 493–500). Tehran, Iran: Copernicus Publications. <a href="https://doi.org/10.5194/isprs-annals-x-4-w8-2025-493-2026">https://doi.org/10.5194/isprs-annals-x-4-w8-2025-493-2026</a>'
  chicago: Eghbali Mardekheh, Masoumeh, Meysam Argany, Farid Karimipour, and Seyed
    Mohammad Sedghitabar. “Real Time Interactive Web GIS Based Modelling of High Traffic
    Air Corridors in Iran Using Origin Destination Matrix Analysis.” In <i>8th ISPRS
    Geospatial Conference</i>, X:493–500. Copernicus Publications, 2026. <a href="https://doi.org/10.5194/isprs-annals-x-4-w8-2025-493-2026">https://doi.org/10.5194/isprs-annals-x-4-w8-2025-493-2026</a>.
  ieee: M. Eghbali Mardekheh, M. Argany, F. Karimipour, and S. M. Sedghitabar, “Real
    time interactive web GIS based modelling of high traffic air corridors in Iran
    using origin destination matrix analysis,” in <i>8th ISPRS Geospatial Conference</i>,
    Tehran, Iran, 2026, vol. X, no. 4/W8-2025, pp. 493–500.
  ista: 'Eghbali Mardekheh M, Argany M, Karimipour F, Sedghitabar SM. 2026. Real time
    interactive web GIS based modelling of high traffic air corridors in Iran using
    origin destination matrix analysis. 8th ISPRS Geospatial Conference. ISPRS: Conference
    on Photogrammetry, Remote Sensing and Spatial Information Sciences, vol. X, 493–500.'
  mla: Eghbali Mardekheh, Masoumeh, et al. “Real Time Interactive Web GIS Based Modelling
    of High Traffic Air Corridors in Iran Using Origin Destination Matrix Analysis.”
    <i>8th ISPRS Geospatial Conference</i>, vol. X, no. 4/W8-2025, Copernicus Publications,
    2026, pp. 493–500, doi:<a href="https://doi.org/10.5194/isprs-annals-x-4-w8-2025-493-2026">10.5194/isprs-annals-x-4-w8-2025-493-2026</a>.
  short: M. Eghbali Mardekheh, M. Argany, F. Karimipour, S.M. Sedghitabar, in:, 8th
    ISPRS Geospatial Conference, Copernicus Publications, 2026, pp. 493–500.
conference:
  end_date: 2025-12-17
  location: Tehran, Iran
  name: 'ISPRS: Conference on Photogrammetry, Remote Sensing and Spatial Information
    Sciences,'
  start_date: 2025-12-15
das_tickbox: '0'
date_created: 2026-07-13T09:51:29Z
date_published: 2026-05-29T00:00:00Z
date_updated: 2026-07-14T05:56:30Z
day: '29'
ddc:
- '500'
department:
- _id: HeEd
doi: 10.5194/isprs-annals-x-4-w8-2025-493-2026
file:
- access_level: open_access
  checksum: 7c088dd179cfee6074a350c95671dbe3
  content_type: application/pdf
  creator: dernst
  date_created: 2026-07-14T05:55:34Z
  date_updated: 2026-07-14T05:55:34Z
  file_id: '22328'
  file_name: 2026_ISPRS_EghbaliMardekheh.pdf
  file_size: 2697680
  relation: main_file
  success: 1
file_date_updated: 2026-07-14T05:55:34Z
has_accepted_license: '1'
issue: -4/W8-2025
keyword:
- Air Traffic simulation
- Dynamic Air Traffic Corridors
- Origin Destination matrix
- Interactive Web GIS
- Iran Aviation Network
- Spatiotemporal Modelling
language:
- iso: eng
month: '05'
oa: 1
oa_version: Published Version
page: 493-500
publication: 8th ISPRS Geospatial Conference
publication_identifier:
  issn:
  - 2194-9050
publication_status: published
publisher: Copernicus Publications
quality_controlled: '1'
researchdata_availability: no
scopus_import: '1'
status: public
supplementarymaterial: no
title: Real time interactive web GIS based modelling of high traffic air corridors
  in Iran using origin destination matrix analysis
tmp:
  image: /images/cc_by.png
  legal_code_url: https://creativecommons.org/licenses/by/4.0/legalcode
  name: Creative Commons Attribution 4.0 International Public License (CC-BY 4.0)
  short: CC BY (4.0)
type: conference
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: X
year: '2026'
...
