---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '23087'
abstract:
- lang: eng
  text: Disordered materials such as glasses are promising candidates as solid-state
    electrolytes for batteries, but they tend to exhibit low ionic conductivity and
    current methods for investigating and predicting the ionic conductivity of electrolyte
    materials are inefficient. Here, we propose a framework that summarizes the topological
    properties of the electrolyte material’s atomic structure with a weighted graph
    based on periodic boundary conditions. We then compute a variation of the max-flow
    algorithm, a commonly used model in continuum models of transportation and liquid
    flow, on this summary and show that it is compatible with the simulated periodic
    atomic structures. Using molecular dynamics simulations of various glassy solid-state
    electrolyte families including both mobile lithium and sodium ions, we validate
    the approach by showing a positive correlation between the area-normalized maximum
    flow predicted from the static glass structures and the ionic conductivity as
    obtained from the simulations, especially in the case of high-conductivity sulfide
    glass electrolytes. We envision that the developed methodology, which only relies
    on static atomic structure, will accelerate the discovery of highly conductive
    sulfide glassy electrolytes for high-performance all-solid-state batteries.
acknowledgement: We thank the Danish e-Infrastructure Cooperation (DeiC) for access
  to computational resources at Sophia and LUMI-C (DeiC-AAU-N5-202200005). This work
  was supported by the Independent Research Fund Denmark (1026-00037), European Union
  (ERC, NewGLASS, 101044664), and Danish Data Science Academy, which in turn is funded
  by the Novo Nordisk Foundation (NNF21SA0069429) and VILLUM FONDEN (40516). Y.B.B.
  acknowledges support from the Austrian Science Fund (FWF) 10.55776/ESP9584724.
article_number: '10343'
article_processing_charge: Yes
article_type: original
author:
- first_name: Matteo
  full_name: Pegoraro, Matteo
  last_name: Pegoraro
- first_name: Rasmus
  full_name: Christensen, Rasmus
  last_name: Christensen
- first_name: Søren S.
  full_name: Sørensen, Søren S.
  last_name: Sørensen
- first_name: Anders R.
  full_name: Lindbjerg, Anders R.
  last_name: Lindbjerg
- first_name: Tao
  full_name: Du, Tao
  last_name: Du
- first_name: Yossi
  full_name: Bleile, Yossi
  id: 920a7385-7995-11ef-9bfd-8c434cd8f3c2
  last_name: Bleile
  orcid: 0000-0002-4861-9174
- first_name: Anne Marie
  full_name: Svane, Anne Marie
  last_name: Svane
- first_name: Christophe A.N.
  full_name: Biscio, Christophe A.N.
  last_name: Biscio
- first_name: Lisbeth
  full_name: Fajstrup, Lisbeth
  last_name: Fajstrup
- first_name: Morten M.
  full_name: Smedskjaer, Morten M.
  last_name: Smedskjaer
citation:
  ama: Pegoraro M, Christensen R, Sørensen SS, et al. Predicting ionic conductivity
    of sulfide glass solid-state electrolytes using max-flow methodology. <i>Nature
    Communications</i>. 2026;17. doi:<a href="https://doi.org/10.1038/s41467-026-77363-w">10.1038/s41467-026-77363-w</a>
  apa: Pegoraro, M., Christensen, R., Sørensen, S. S., Lindbjerg, A. R., Du, T., Bokor
    Bleile, Y., … Smedskjaer, M. M. (2026). Predicting ionic conductivity of sulfide
    glass solid-state electrolytes using max-flow methodology. <i>Nature Communications</i>.
    Springer Nature. <a href="https://doi.org/10.1038/s41467-026-77363-w">https://doi.org/10.1038/s41467-026-77363-w</a>
  chicago: Pegoraro, Matteo, Rasmus Christensen, Søren S. Sørensen, Anders R. Lindbjerg,
    Tao Du, Yossi Bokor Bleile, Anne Marie Svane, Christophe A.N. Biscio, Lisbeth
    Fajstrup, and Morten M. Smedskjaer. “Predicting Ionic Conductivity of Sulfide
    Glass Solid-State Electrolytes Using Max-Flow Methodology.” <i>Nature Communications</i>.
    Springer Nature, 2026. <a href="https://doi.org/10.1038/s41467-026-77363-w">https://doi.org/10.1038/s41467-026-77363-w</a>.
  ieee: M. Pegoraro <i>et al.</i>, “Predicting ionic conductivity of sulfide glass
    solid-state electrolytes using max-flow methodology,” <i>Nature Communications</i>,
    vol. 17. Springer Nature, 2026.
  ista: Pegoraro M, Christensen R, Sørensen SS, Lindbjerg AR, Du T, Bokor Bleile Y,
    Svane AM, Biscio CAN, Fajstrup L, Smedskjaer MM. 2026. Predicting ionic conductivity
    of sulfide glass solid-state electrolytes using max-flow methodology. Nature Communications.
    17, 10343.
  mla: Pegoraro, Matteo, et al. “Predicting Ionic Conductivity of Sulfide Glass Solid-State
    Electrolytes Using Max-Flow Methodology.” <i>Nature Communications</i>, vol. 17,
    10343, Springer Nature, 2026, doi:<a href="https://doi.org/10.1038/s41467-026-77363-w">10.1038/s41467-026-77363-w</a>.
  short: M. Pegoraro, R. Christensen, S.S. Sørensen, A.R. Lindbjerg, T. Du, Y. Bokor
    Bleile, A.M. Svane, C.A.N. Biscio, L. Fajstrup, M.M. Smedskjaer, Nature Communications
    17 (2026).
das_tickbox: '1'
dataavailabilitystatement: All data supporting the findings of this study are available
  within the article and Supplementary Information files. Source data are provided
  with this paper. The developed code to perform the max-flow calculations is available
  as part of the Topological Materials Analysis (ToMA) library, which is available
  at Zenodo (https://doi.org/10.5281/zenodo.10781424) and Github (https://github.com/yossibokorbleile/TopologicalMaterialAnalysis),
  with documentation available at https://yossi.eu/toma/. To enhance usability, we
  have included a brief documentation on how to compile ToMA as well as a minimal
  working example of the code together with an example trajectory directly in the
  ToMA repository. LAMMPS is an open-source code available at https://lammps.sandia.gov.
date_created: 2026-10-11T22:02:03Z
date_published: 2026-09-30T00:00:00Z
date_updated: 2026-10-12T09:03:58Z
day: '30'
ddc:
- '500'
department:
- _id: HeEd
doi: 10.1038/s41467-026-77363-w
external_id:
  pmid:
  - '42811056'
file:
- access_level: open_access
  checksum: eba760f5982a89f59664957e00c5d2d6
  content_type: application/pdf
  creator: dernst
  date_created: 2026-10-12T09:00:06Z
  date_updated: 2026-10-12T09:00:06Z
  file_id: '23104'
  file_name: 2026_NatureComm_Pegoraro.pdf
  file_size: 1889857
  relation: main_file
  success: 1
file_date_updated: 2026-10-12T09:00:06Z
fulldoi: https://doi.org/10.1038/s41467-026-77363-w
has_accepted_license: '1'
intvolume: '        17'
language:
- iso: eng
month: '09'
oa: 1
oa_version: Published Version
pmid: 1
project:
- _id: 9106a876-16d5-11f0-9cad-bbf11c9952f9
  grant_number: ESP 9584724
  name: Quantitative Unbiased Shape Analysis with Geometry &amp; Topology
publication: Nature Communications
publication_identifier:
  eissn:
  - 2041-1723
publication_status: published
publisher: Springer Nature
quality_controlled: '1'
researchdata_availability: yes
scopus_import: '1'
status: public
supplementarymaterial: yes
title: Predicting ionic conductivity of sulfide glass solid-state electrolytes using
  max-flow methodology
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: 17
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '23091'
abstract:
- lang: eng
  text: Glaciers worldwide are becoming increasingly debris-covered, yet many aspects
    within the coupled glacier-debris system are not well-understood. While the insulating
    effect of continuous debris layers is well-known, the transient feedbacks with
    glacier dynamics are poorly understood. The main aim of this study is to better
    understand the complex transient glacier response and debris-induced feedbacks
    through numerical flow modelling. We present an improved flowline model that couples
    ice flow, depth-resolved debris transport, and debris cover impact on mass balance.
    This approach allows for a detailed examination of the dynamics of debris-covered
    glaciers under transient forcing conditions of climate and debris input over extended
    timescales. Our results indicate that low-amplitude, decade-scale variability
    in debris or climate forcing does not substantially impact glacier evolution.
    However, large debris supply events can have a sustained impact. We find that
    debris-covered glacier response to warming climate forcing is non-monotonic, with
    distinct phases of thinning, retreat, and long-term re-advance. We attribute this
    to a separate, longer timescale process of englacial debris transport. Additionally,
    feedbacks in the englacial debris trajectory and complex bed topography further
    amplify the non-linear pattern of retreat in the transient glacier response to
    warming.
acknowledgement: We thank Evan Miles, Ramachandran Shankar, and Argha Banerjee for
  valuable discussions and inputs on experiment design and analysis. This research
  has been mainly funded by the SNSF (grant no. IZINZ2_209521) within the Indo-Swiss
  joint trilateral SNSF-ICSSR-MoES scheme and the earlier SNSF (grant no. 200021_169775).
article_processing_charge: Yes
article_type: original
author:
- first_name: Florian
  full_name: Hardmeier, Florian
  last_name: Hardmeier
- first_name: James
  full_name: Ferguson, James
  id: 05fd8d9b-bd43-11eb-8d36-f8fb1cc98040
  last_name: Ferguson
- first_name: Andreas
  full_name: Vieli, Andreas
  last_name: Vieli
citation:
  ama: Hardmeier F, Ferguson J, Vieli A. Feedbacks and timescales in the modelled
    transient response of debris-covered glaciers. <i>The Cryosphere</i>. 2026;20(9):5365-5392.
    doi:<a href="https://doi.org/10.5194/tc-20-5365-2026">10.5194/tc-20-5365-2026</a>
  apa: Hardmeier, F., Ferguson, J., &#38; Vieli, A. (2026). Feedbacks and timescales
    in the modelled transient response of debris-covered glaciers. <i>The Cryosphere</i>.
    Copernicus Publications. <a href="https://doi.org/10.5194/tc-20-5365-2026">https://doi.org/10.5194/tc-20-5365-2026</a>
  chicago: Hardmeier, Florian, James Ferguson, and Andreas Vieli. “Feedbacks and Timescales
    in the Modelled Transient Response of Debris-Covered Glaciers.” <i>The Cryosphere</i>.
    Copernicus Publications, 2026. <a href="https://doi.org/10.5194/tc-20-5365-2026">https://doi.org/10.5194/tc-20-5365-2026</a>.
  ieee: F. Hardmeier, J. Ferguson, and A. Vieli, “Feedbacks and timescales in the
    modelled transient response of debris-covered glaciers,” <i>The Cryosphere</i>,
    vol. 20, no. 9. Copernicus Publications, pp. 5365–5392, 2026.
  ista: Hardmeier F, Ferguson J, Vieli A. 2026. Feedbacks and timescales in the modelled
    transient response of debris-covered glaciers. The Cryosphere. 20(9), 5365–5392.
  mla: Hardmeier, Florian, et al. “Feedbacks and Timescales in the Modelled Transient
    Response of Debris-Covered Glaciers.” <i>The Cryosphere</i>, vol. 20, no. 9, Copernicus
    Publications, 2026, pp. 5365–92, doi:<a href="https://doi.org/10.5194/tc-20-5365-2026">10.5194/tc-20-5365-2026</a>.
  short: F. Hardmeier, J. Ferguson, A. Vieli, The Cryosphere 20 (2026) 5365–5392.
das_tickbox: '1'
dataavailabilitystatement: 'The model presented in this study as well as the code
  and synthetic data (generated from model runs) are available on Zenodo: https://doi.org/10.5281/zenodo.22687411
  (Hardmeier et al., 2026). Two animations, referenced to in the text as Video Supplement
  1 and 2, are available on Zenodo: https://doi.org/10.5281/zenodo.22687411 (Hardmeier
  et al., 2026).'
date_created: 2026-10-11T22:02:04Z
date_published: 2026-09-21T00:00:00Z
date_updated: 2026-10-12T09:21:04Z
day: '21'
ddc:
- '550'
- '000'
department:
- _id: TiVo
doi: 10.5194/tc-20-5365-2026
file:
- access_level: open_access
  checksum: b934b69f66efac91c08680a513bf74d9
  content_type: application/pdf
  creator: dernst
  date_created: 2026-10-12T09:17:51Z
  date_updated: 2026-10-12T09:17:51Z
  file_id: '23105'
  file_name: 2026_Cryosphere_Hardmeier.pdf
  file_size: 9284677
  relation: main_file
  success: 1
file_date_updated: 2026-10-12T09:17:51Z
fulldoi: https://doi.org/10.5194/tc-20-5365-2026
has_accepted_license: '1'
intvolume: '        20'
issue: '9'
language:
- iso: eng
month: '09'
oa: 1
oa_version: None
page: 5365-5392
publication: The Cryosphere
publication_identifier:
  eissn:
  - 1994-0424
  issn:
  - 1994-0416
publication_status: published
publisher: Copernicus Publications
quality_controlled: '1'
researchdata_availability: yes
scopus_import: '1'
status: public
supplementarymaterial: yes
title: Feedbacks and timescales in the modelled transient response of debris-covered
  glaciers
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: 20
year: '2026'
...
---
OA_place: repository
OA_type: green
_id: '23057'
abstract:
- lang: eng
  text: "We recently showed that macroscopic nuclear spin ensembles prepared in coherent
    spin states can dramatically enhance the interaction rates of weakly interacting
    cosmic relics, such as dark matter and the cosmic neutrino background, through
    collective quantum effects analogous to Dicke superradiance, where the deexcitation
    and excitation rates scale as the square of the number of spins \U0001D4412. We
    thus coined these processes superradiant interactions. In this paper, we propose
    a protocol to realize this enhancement and boost the discovery potential for such
    relics. We show how concepts from quantum optics can be adapted to nuclear spins
    coupled to superconducting circuits, enabling high-sensitivity systems. The spins
    are first initialized into a coherent spin state via a \U0001D70B/2 Rabi pulse
    from the ground state. When the circuit is sufficiently detuned from resonance,
    the spin-circuit interaction implements a squeezing Hamiltonian. Because squeezing
    must outpace spin relaxation and dephasing, the protocol favors macroscopic ensembles
    and high-quality superconducting circuits. During this squeezing phase, the standard
    quantum variance is reduced by up to 4.8 orders of magnitude, equivalent to 48
    dB of squeezing, for circuits with quality factors \U0001D444∼10^8–10^9. The signal
    imprinted on the spins during the squeezing protocol can be magnified by further
    utilizing the squeezing interactions, easing the requirement for shot-noise-limited
    readout. This protocol has the potential to significantly accelerate axion and
    dark photon dark matter searches and extend the reach of existing axion experiments
    to probe QCD axion-nuclear spin couplings. More broadly, it paves the way for
    detecting coherent inelastic interactions from other cosmic relics, most notably
    the cosmic neutrino background, and establishes nuclear-spin-based systems as
    a class of quantum, ultra-low-threshold detectors."
acknowledgement: We are grateful to K. Irwin for illuminating discussions, and M.
  Schleier-Smith, M. Kasevich, J. Hogan, N. Rapidis, M. Fedderke, A. Geraci, G. Gratta,
  D. Schuster, D. Budker, and A. Sushkov for very valuable conversations. O.H. acknowledges
  support by the Institute of Science and Technology Austria (ISTA). A.A., S.D., and
  M.G. acknowledge the hospitality provided by ISTA, where part of this work was being
  completed. A.A., M.G., and O.H. acknowledge the hospitality provided by the Leinweber
  Institute for Theoretical Physics at Stanford, where part of this work was being
  completed. S.D. acknowledges support by NSF Grant No. PHY-2310429 and the Gordon
  and Betty Moore Foundation Grant No. GBMF7946, and Perimeter Institute and its hospitality.
  Research at Perimeter Institute is supported in part by the Government of Canada
  through the Department of Innovation, Science and Economic Development and by the
  Province of Ontario through the Ministry of Colleges and Universities. A.A. is grateful
  for the support of the Stavros Niarchos Foundation.
article_number: '063714'
article_processing_charge: No
article_type: original
arxiv: 1
author:
- first_name: Marios
  full_name: Galanis, Marios
  last_name: Galanis
- first_name: Onur
  full_name: Hosten, Onur
  id: 4C02D85E-F248-11E8-B48F-1D18A9856A87
  last_name: Hosten
  orcid: 0000-0002-2031-204X
- first_name: Asimina
  full_name: Arvanitaki, Asimina
  last_name: Arvanitaki
- first_name: Savas
  full_name: Dimopoulos, Savas
  last_name: Dimopoulos
citation:
  ama: Galanis M, Hosten O, Arvanitaki A, Dimopoulos S. Superradiant interactions
    for relic detection with entangled nuclear spins. <i>Physical Review A</i>. 2026;113(6).
    doi:<a href="https://doi.org/10.1103/Z2D9-4GV6">10.1103/Z2D9-4GV6</a>
  apa: Galanis, M., Hosten, O., Arvanitaki, A., &#38; Dimopoulos, S. (2026). Superradiant
    interactions for relic detection with entangled nuclear spins. <i>Physical Review
    A</i>. American Physical Society. <a href="https://doi.org/10.1103/Z2D9-4GV6">https://doi.org/10.1103/Z2D9-4GV6</a>
  chicago: Galanis, Marios, Onur Hosten, Asimina Arvanitaki, and Savas Dimopoulos.
    “Superradiant Interactions for Relic Detection with Entangled Nuclear Spins.”
    <i>Physical Review A</i>. American Physical Society, 2026. <a href="https://doi.org/10.1103/Z2D9-4GV6">https://doi.org/10.1103/Z2D9-4GV6</a>.
  ieee: M. Galanis, O. Hosten, A. Arvanitaki, and S. Dimopoulos, “Superradiant interactions
    for relic detection with entangled nuclear spins,” <i>Physical Review A</i>, vol.
    113, no. 6. American Physical Society, 2026.
  ista: Galanis M, Hosten O, Arvanitaki A, Dimopoulos S. 2026. Superradiant interactions
    for relic detection with entangled nuclear spins. Physical Review A. 113(6), 063714.
  mla: Galanis, Marios, et al. “Superradiant Interactions for Relic Detection with
    Entangled Nuclear Spins.” <i>Physical Review A</i>, vol. 113, no. 6, 063714, American
    Physical Society, 2026, doi:<a href="https://doi.org/10.1103/Z2D9-4GV6">10.1103/Z2D9-4GV6</a>.
  short: M. Galanis, O. Hosten, A. Arvanitaki, S. Dimopoulos, Physical Review A 113
    (2026).
corr_author: '1'
das_tickbox: '1'
dataavailabilitystatement: The data that support the findings of this article are
  not publicly available. The data are available from the authors upon reasonable
  request.
date_created: 2026-10-04T22:01:57Z
date_published: 2026-06-01T00:00:00Z
date_updated: 2026-10-12T08:36:40Z
day: '01'
department:
- _id: OnHo
doi: 10.1103/Z2D9-4GV6
external_id:
  arxiv:
  - '2508.20520'
fulldoi: https://doi.org/10.1103/Z2D9-4GV6
intvolume: '       113'
issue: '6'
language:
- iso: eng
main_file_link:
- open_access: '1'
  url: https://doi.org/10.48550/arXiv.2508.20520
month: '06'
oa: 1
oa_version: Preprint
publication: Physical Review A
publication_identifier:
  eissn:
  - 2469-9934
  issn:
  - 2469-9926
publication_status: published
publisher: American Physical Society
quality_controlled: '1'
researchdata_availability: upon request
scopus_import: '1'
status: public
supplementarymaterial: yes
title: Superradiant interactions for relic detection with entangled nuclear spins
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 113
year: '2026'
...
---
OA_type: closed access
_id: '23086'
abstract:
- lang: eng
  text: The division of a mother cell into two daughter cells is a fundamental process
    in biology, involving the transfer of genomic information to the next generation
    of cells. In plant roots, cell divisions occur in the root apical meristem, a
    specialized tissue located at the plant’s root tip. Cell proliferation rates in
    the root apical meristem shape root growth, thereby contributing to general development
    as well as the acclimatization to stressful environmental conditions through phenotypic
    plasticity. Here, we present a protocol for the microscopical analysis of cell
    proliferation in Arabidopsis thaliana root meristems by 5-ethynyl-2ʹ-deoxyuridine
    (EdU) staining. EdU, a thymine-analog, is incorporated into newly synthesized
    DNA of proliferative cells during the S-phase of the cell cycle. Subsequently,
    EdU-containing nuclei can be labeled with a fluorophore and detected by confocal
    laser scanning microscopy. The combination of the EdU assay with cell wall staining
    enables the quantification of root meristem architecture parameters and cell division
    activity from microscopic images. Together, this can elucidate how root meristems
    respond to changes in environmental conditions or address fundamental questions
    of developmental plant biology.
alternative_title:
- Methods in Molecular Biology
article_processing_charge: No
author:
- first_name: Tilman
  full_name: Jacob, Tilman
  last_name: Jacob
- first_name: Haiyue
  full_name: Ai, Haiyue
  id: 71a6871f-c08f-11ee-886c-c975579c368c
  last_name: Ai
- first_name: Marcel
  full_name: Quint, Marcel
  last_name: Quint
citation:
  ama: 'Jacob T, Ai H, Quint M. EdU-Based Quantitative Analysis of Cell Proliferation
    in Arabidopsis Root Meristems. In: <i>Root Development</i>. Vol 3086. MIMB. New
    York: Springer; 2026:165-176. doi:<a href="https://doi.org/10.1007/978-1-0716-5603-7_13">10.1007/978-1-0716-5603-7_13</a>'
  apa: 'Jacob, T., Ai, H., &#38; Quint, M. (2026). EdU-Based Quantitative Analysis
    of Cell Proliferation in Arabidopsis Root Meristems. In <i>Root Development</i>
    (Vol. 3086, pp. 165–176). New York: Springer. <a href="https://doi.org/10.1007/978-1-0716-5603-7_13">https://doi.org/10.1007/978-1-0716-5603-7_13</a>'
  chicago: 'Jacob, Tilman, Haiyue Ai, and Marcel Quint. “EdU-Based Quantitative Analysis
    of Cell Proliferation in Arabidopsis Root Meristems.” In <i>Root Development</i>,
    3086:165–76. MIMB. New York: Springer, 2026. <a href="https://doi.org/10.1007/978-1-0716-5603-7_13">https://doi.org/10.1007/978-1-0716-5603-7_13</a>.'
  ieee: 'T. Jacob, H. Ai, and M. Quint, “EdU-Based Quantitative Analysis of Cell Proliferation
    in Arabidopsis Root Meristems,” in <i>Root Development</i>, vol. 3086, New York:
    Springer, 2026, pp. 165–176.'
  ista: 'Jacob T, Ai H, Quint M. 2026.EdU-Based Quantitative Analysis of Cell Proliferation
    in Arabidopsis Root Meristems. In: Root Development. Methods in Molecular Biology,
    vol. 3086, 165–176.'
  mla: Jacob, Tilman, et al. “EdU-Based Quantitative Analysis of Cell Proliferation
    in Arabidopsis Root Meristems.” <i>Root Development</i>, vol. 3086, Springer,
    2026, pp. 165–76, doi:<a href="https://doi.org/10.1007/978-1-0716-5603-7_13">10.1007/978-1-0716-5603-7_13</a>.
  short: T. Jacob, H. Ai, M. Quint, in:, Root Development, Springer, New York, 2026,
    pp. 165–176.
date_created: 2026-10-11T22:02:03Z
date_published: 2026-10-01T00:00:00Z
date_updated: 2026-10-12T09:13:28Z
day: '01'
department:
- _id: JiFr
doi: 10.1007/978-1-0716-5603-7_13
external_id:
  pmid:
  - '42814359'
fulldoi: https://doi.org/10.1007/978-1-0716-5603-7_13
intvolume: '      3086'
keyword:
- Root growth
- Root development
- Root meristem
- Cell cycle
- Cell division
- S-phase
- EdU
- Arabidopsis thaliana
- Microscopy
language:
- iso: eng
month: '10'
oa_version: None
page: 165-176
place: New York
pmid: 1
publication: Root Development
publication_identifier:
  eisbn:
  - '9781071656037'
  eissn:
  - 1940-6029
publication_status: published
publisher: Springer
quality_controlled: '1'
scopus_import: '1'
series_title: MIMB
status: public
title: EdU-Based Quantitative Analysis of Cell Proliferation in Arabidopsis Root Meristems
type: book_chapter
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 3086
year: '2026'
...
---
OA_type: closed access
_id: '23056'
abstract:
- lang: eng
  text: Superconducting qubits face scaling challenges due to millikelvin temperature
    requirements. Here we demonstrate the generation and low-noise upconversion of
    single microwave photons to telecom frequencies, paving the way for quantum networks
    with superconducting qubits.
alternative_title:
- Technical Digest Series
article_number: QM2A.1
article_processing_charge: No
author:
- first_name: Andrei
  full_name: Militaru, Andrei
  id: d67706f8-8eb1-11ee-ad1b-9c30dfa19e0b
  last_name: Militaru
- first_name: Thomas
  full_name: Werner, Thomas
  id: 1fcd8497-dba3-11ea-a45e-c6fbd715f7c7
  last_name: Werner
  orcid: 0009-0001-2346-5236
- first_name: Erfan
  full_name: Riyazi, Erfan
  id: 53322f94-5355-11ee-ae5a-ff6f81c87d51
  last_name: Riyazi
- first_name: Samarth
  full_name: Hawaldar, Samarth
  id: 221708e1-1ff6-11ee-9fa6-85146607433e
  last_name: Hawaldar
  orcid: 0000-0002-1965-4309
- first_name: Rishabh
  full_name: Sahu, Rishabh
  id: 47D26E34-F248-11E8-B48F-1D18A9856A87
  last_name: Sahu
  orcid: 0000-0001-6264-2162
- first_name: Georg M
  full_name: Arnold, Georg M
  id: 3770C838-F248-11E8-B48F-1D18A9856A87
  last_name: Arnold
  orcid: 0000-0003-1397-7876
- first_name: Paul
  full_name: Falthansl-Scheinecker, Paul
  id: 85b43b21-15b2-11ec-abd3-e2c252cc2285
  last_name: Falthansl-Scheinecker
- first_name: Jennifer Anais
  full_name: Sanchez Naranjo, Jennifer Anais
  id: 0fd10295-ebd4-11ec-b0f1-c1c8465143f9
  last_name: Sanchez Naranjo
- first_name: Dante
  full_name: Loi, Dante
  id: a24803ec-c619-11f1-873b-95804e96f22f
  last_name: Loi
- first_name: Lucky
  full_name: Kapoor, Lucky
  id: 84b9700b-15b2-11ec-abd3-831089e67615
  last_name: Kapoor
  orcid: 0000-0001-8319-2148
- first_name: Martin
  full_name: Zemlicka, Martin
  id: 2DCF8DE6-F248-11E8-B48F-1D18A9856A87
  last_name: Zemlicka
  orcid: 0009-0005-0878-3032
- first_name: Liu
  full_name: Qiu, Liu
  id: 45e99c0d-1eb1-11eb-9b96-ed8ab2983cac
  last_name: Qiu
  orcid: 0000-0003-4345-4267
- first_name: Johannes M
  full_name: Fink, Johannes M
  id: 4B591CBA-F248-11E8-B48F-1D18A9856A87
  last_name: Fink
  orcid: 0000-0001-8112-028X
citation:
  ama: 'Militaru A, Werner T, Riyazi E, et al. Electro-optic conversion of itinerant
    Fock states. In: <i>Quantum 2.0 Conference and Exhibition</i>. Optica Publishing
    Group; 2026.'
  apa: 'Militaru, A., Werner, T., Riyazi, E., Hawaldar, S., Sahu, R., Arnold, G. M.,
    … Fink, J. M. (2026). Electro-optic conversion of itinerant Fock states. In <i>Quantum
    2.0 Conference and Exhibition</i>. Glasgow, United Kingdom: Optica Publishing
    Group.'
  chicago: Militaru, Andrei, Thomas Werner, Erfan Riyazi, Samarth Hawaldar, Rishabh
    Sahu, Georg M Arnold, Paul Falthansl-Scheinecker, et al. “Electro-Optic Conversion
    of Itinerant Fock States.” In <i>Quantum 2.0 Conference and Exhibition</i>. Optica
    Publishing Group, 2026.
  ieee: A. Militaru <i>et al.</i>, “Electro-optic conversion of itinerant Fock states,”
    in <i>Quantum 2.0 Conference and Exhibition</i>, Glasgow, United Kingdom, 2026.
  ista: Militaru A, Werner T, Riyazi E, Hawaldar S, Sahu R, Arnold GM, Falthansl-Scheinecker
    P, Sanchez Naranjo JA, Loi D, Kapoor L, Zemlicka M, Qiu L, Fink JM. 2026. Electro-optic
    conversion of itinerant Fock states. Quantum 2.0 Conference and Exhibition. Quantum
    2.0, Technical Digest Series, , QM2A.1.
  mla: Militaru, Andrei, et al. “Electro-Optic Conversion of Itinerant Fock States.”
    <i>Quantum 2.0 Conference and Exhibition</i>, QM2A.1, Optica Publishing Group,
    2026.
  short: A. Militaru, T. Werner, E. Riyazi, S. Hawaldar, R. Sahu, G.M. Arnold, P.
    Falthansl-Scheinecker, J.A. Sanchez Naranjo, D. Loi, L. Kapoor, M. Zemlicka, L.
    Qiu, J.M. Fink, in:, Quantum 2.0 Conference and Exhibition, Optica Publishing
    Group, 2026.
conference:
  end_date: 2026-06-18
  location: Glasgow, United Kingdom
  name: Quantum 2.0
  start_date: 2026-06-15
corr_author: '1'
date_created: 2026-10-04T22:01:57Z
date_published: 2026-09-01T00:00:00Z
date_updated: 2026-10-12T08:53:25Z
day: '01'
department:
- _id: JoFi
- _id: GradSch
- _id: GeKa
language:
- iso: eng
month: '09'
oa_version: None
publication: Quantum 2.0 Conference and Exhibition
publication_identifier:
  isbn:
  - '9781957171616'
publication_status: published
publisher: Optica Publishing Group
scopus_import: '1'
status: public
title: Electro-optic conversion of itinerant Fock states
type: conference
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '23092'
abstract:
- lang: eng
  text: We present the number density of massive (log(M*/Mo)> 10.3) quiescent galaxies
    at 2 < z < 5 using JWST NIRSpec PRISM spectra. This work relies on spectra from
    RUBIES, which provides excellent data quality and an unparalleled, well-defined
    targeting strategy to robustly infer physical properties and number densities.
    We identify quiescent galaxy candidates within RUBIES through principal component
    analysis and construct a final sample using star formation histories derived from
    spectrophotometric fitting of the NIRSpec PRISM spectra and NIRCam photometry.
    By inverting the RUBIES selection function, we correct for survey incompleteness
    and calculate the number density of massive quiescent galaxies at these redshifts,
    providing the most complete spectroscopic estimates prior to cosmic noon to date.
    We find that early massive quiescent galaxies are surprisingly common (≳10−5 Mpc−3
    by 4 < z < 5), which is consistent with previous studies based on JWST photometry
    alone and/or in smaller survey areas. We compare our number densities with predictions
    from six state-of-the-art cosmological galaxy formation simulations. At z > 3,
    most simulations fail to produce enough massive quiescent galaxies, suggesting
    the treatment of feedback and/or the channels for early efficient formation are
    incomplete in most galaxy evolution models.
acknowledgement: "We thank Alan Pearl for his contribution to estimating the cosmic
  variance contribution to the number density uncertainties in this work. We thank
  Hans-Walter Rix for the valuable discussion on the selection function and correcting
  the spectroscopic incompleteness of massive quiescent galaxies in RUBIES.\r\n\r\nSome
  of the data products presented herein were retrieved from the Dawn JWST Archive
  (DJA). DJA is an initiative of the Cosmic Dawn Center (DAWN), which is funded by
  the Danish National Research Foundation under grant DNRF140.\r\n\r\nThe Cosmic Dawn
  Center is funded by the Danish National Research Foundation (DNRF) under grant #140.\r\n\r\nSupport
  for this work was provided by The Brinson Foundation through a Brinson Prize Fellowship
  grant.\r\n\r\nR.B. gratefully acknowledges support from the Research Corporation
  for Scientific Advancement (RCSA) Cottrell Scholar Award ID No: 27587.\r\n\r\nThe
  work of C.C.W. is supported by NOIRLab, which is managed by the Association of Universities
  for Research in Astronomy (AURA) under a cooperative agreement with the National
  Science Foundation.\r\n\r\nT.B.M. was supported by a CIERA Postdoctoral Fellowship.\r\n\r\nThis
  work is based in part on observations made with the NASA/ESA/CSA James Webb Space
  Telescope. The data were obtained from the Mikulski Archive for Space Telescopes
  at the Space Telescope Science Institute, which is operated by the Association of
  Universities for Research in Astronomy, Inc., under NASA contract NAS 5-03127 for
  JWST. These observations are associated with program numbers 1180, 1181, 1210, 1211,
  1213, 1214, 1215, 1286, 1345, 1433, 1747, 2028, 2073, 2198, 2282, 2561, 2565, 2750,
  2756, 2767, 3073, 3215, 4233, 4446, 4557, 6368, 6541, and 6585. The specific observations
  analyzed can be accessed via DOI: 10.17909/sjsj-8p46.\r\n\r\nSupport for program
  No. 4233 was provided by NASA through a grant from the Space Telescope Science Institute,
  which is operated by the Association of Universities for Research in Astronomy,
  Inc., under NASA contract NAS 5-03127.\r\n\r\nThe authors acknowledge the CEERS
  and PRIMER teams for developing their observing program with a zero-exclusive access
  period.\r\n\r\nFacility: JWST - James Webb Space Telescope.\r\n\r\nSoftware: Astropy
  (Astropy Collaboration et al. 2013, 2018, 2022), Scipy (P. Virtanen et al. 2020),
  Photutils (L. Bradley 2023), SpectRes (A. C. Carnall 2017), Scikit-learn (F. Pedregosa
  et al. 2011), Prospector (B. Johnson & J. Leja 2017; J. Leja et al. 2017; B. Johnson
  et al. 2021)."
article_number: '252'
article_processing_charge: Yes
article_type: original
arxiv: 1
author:
- first_name: Yunchong
  full_name: Zhang, Yunchong
  last_name: Zhang
- first_name: Anna
  full_name: De Graaff, Anna
  last_name: De Graaff
- first_name: David J.
  full_name: Setton, David J.
  last_name: Setton
- first_name: Sedona H.
  full_name: Price, Sedona H.
  last_name: Price
- first_name: Rachel
  full_name: Bezanson, Rachel
  last_name: Bezanson
- first_name: Claudia
  full_name: Del P. Lagos, Claudia
  last_name: Del P. Lagos
- first_name: Sam E.
  full_name: Cutler, Sam E.
  last_name: Cutler
- first_name: Ian
  full_name: Mcconachie, Ian
  last_name: Mcconachie
- first_name: Nikko J.
  full_name: Cleri, Nikko J.
  last_name: Cleri
- first_name: Olivia R.
  full_name: Cooper, Olivia R.
  last_name: Cooper
- first_name: Rashmi
  full_name: Gottumukkala, Rashmi
  last_name: Gottumukkala
- first_name: Jenny E.
  full_name: Greene, Jenny E.
  last_name: Greene
- first_name: Michaela
  full_name: Hirschmann, Michaela
  last_name: Hirschmann
- first_name: Gourav
  full_name: Khullar, Gourav
  last_name: Khullar
- first_name: Ivo
  full_name: Labbe, Ivo
  last_name: Labbe
- first_name: Joel
  full_name: Leja, Joel
  last_name: Leja
- first_name: Michael V.
  full_name: Maseda, Michael V.
  last_name: Maseda
- 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: Tim B.
  full_name: Miller, Tim B.
  last_name: Miller
- first_name: Themiya
  full_name: Nanayakkara, Themiya
  last_name: Nanayakkara
- first_name: Katherine A.
  full_name: Suess, Katherine A.
  last_name: Suess
- first_name: Bingjie
  full_name: Wang, Bingjie
  last_name: Wang
- first_name: Katherine E.
  full_name: Whitaker, Katherine E.
  last_name: Whitaker
- first_name: Christina C.
  full_name: Williams, Christina C.
  last_name: Williams
citation:
  ama: Zhang Y, De Graaff A, Setton DJ, et al. RUBIES spectroscopically confirms the
    high number density of quiescent galaxies from2&#60;z&#60;5. <i>The Astrophysical
    Journal</i>. 2026;997(2). doi:<a href="https://doi.org/10.3847/1538-4357/ae24e1">10.3847/1538-4357/ae24e1</a>
  apa: Zhang, Y., De Graaff, A., Setton, D. J., Price, S. H., Bezanson, R., Del P.
    Lagos, C., … Williams, C. C. (2026). RUBIES spectroscopically confirms the high
    number density of quiescent galaxies from2&#60;z&#60;5. <i>The Astrophysical Journal</i>.
    IOP Publishing. <a href="https://doi.org/10.3847/1538-4357/ae24e1">https://doi.org/10.3847/1538-4357/ae24e1</a>
  chicago: Zhang, Yunchong, Anna De Graaff, David J. Setton, Sedona H. Price, Rachel
    Bezanson, Claudia Del P. Lagos, Sam E. Cutler, et al. “RUBIES Spectroscopically
    Confirms the High Number Density of Quiescent Galaxies From2&#60;z&#60;5.” <i>The
    Astrophysical Journal</i>. IOP Publishing, 2026. <a href="https://doi.org/10.3847/1538-4357/ae24e1">https://doi.org/10.3847/1538-4357/ae24e1</a>.
  ieee: Y. Zhang <i>et al.</i>, “RUBIES spectroscopically confirms the high number
    density of quiescent galaxies from2&#60;z&#60;5,” <i>The Astrophysical Journal</i>,
    vol. 997, no. 2. IOP Publishing, 2026.
  ista: Zhang Y, De Graaff A, Setton DJ, Price SH, Bezanson R, Del P. Lagos C, Cutler
    SE, Mcconachie I, Cleri NJ, Cooper OR, Gottumukkala R, Greene JE, Hirschmann M,
    Khullar G, Labbe I, Leja J, Maseda MV, Matthee JJ, Miller TB, Nanayakkara T, Suess
    KA, Wang B, Whitaker KE, Williams CC. 2026. RUBIES spectroscopically confirms
    the high number density of quiescent galaxies from2&#60;z&#60;5. The Astrophysical
    Journal. 997(2), 252.
  mla: Zhang, Yunchong, et al. “RUBIES Spectroscopically Confirms the High Number
    Density of Quiescent Galaxies From2&#60;z&#60;5.” <i>The Astrophysical Journal</i>,
    vol. 997, no. 2, 252, IOP Publishing, 2026, doi:<a href="https://doi.org/10.3847/1538-4357/ae24e1">10.3847/1538-4357/ae24e1</a>.
  short: Y. Zhang, A. De Graaff, D.J. Setton, S.H. Price, R. Bezanson, C. Del P. Lagos,
    S.E. Cutler, I. Mcconachie, N.J. Cleri, O.R. Cooper, R. Gottumukkala, J.E. Greene,
    M. Hirschmann, G. Khullar, I. Labbe, J. Leja, M.V. Maseda, J.J. Matthee, T.B.
    Miller, T. Nanayakkara, K.A. Suess, B. Wang, K.E. Whitaker, C.C. Williams, The
    Astrophysical Journal 997 (2026).
date_created: 2026-10-11T22:02:05Z
date_published: 2026-02-01T00:00:00Z
date_updated: 2026-10-12T11:55:05Z
day: '01'
ddc:
- '520'
department:
- _id: JoMa
doi: 10.3847/1538-4357/ae24e1
external_id:
  arxiv:
  - '2508.08577'
file:
- access_level: open_access
  checksum: 547c63f9265be5d41efdc555a25423cc
  content_type: application/pdf
  creator: dernst
  date_created: 2026-10-12T11:51:24Z
  date_updated: 2026-10-12T11:51:24Z
  file_id: '23110'
  file_name: 2026_AstrophysicalJour_Zhang.pdf
  file_size: 5995619
  relation: main_file
  success: 1
file_date_updated: 2026-10-12T11:51:24Z
fulldoi: https://doi.org/10.3847/1538-4357/ae24e1
has_accepted_license: '1'
intvolume: '       997'
issue: '2'
language:
- iso: eng
month: '02'
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'
scopus_import: '1'
status: public
title: RUBIES spectroscopically confirms the high number density of quiescent galaxies
  from2<z<5
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: 997
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '23093'
abstract:
- lang: eng
  text: Land-use change, such as the transformation of woody ecosystems into open
    pastures, acts as a strong ecological filter, favouring some species while excluding
    others according to differences in ecological niche breadth. Understanding how
    differences in niche breadth influence species responses under anthropogenic filters
    is crucial to anticipate their persistence or displacement. In this study, we
    quantified realized niche breadth in two sympatric ecosystem engineers, the Neotropical
    leaf-cutter ants Atta cephalotes and Atta laevigata, to test whether breadth differences
    are consistent with specialist and generalist ecological strategies. We characterized
    realized niche breadth across fine-scale environmental gradients by integrating
    hemispherical photography, microclimatic data, mound architecture, and edaphic
    profiles from 114 colonies across a regional transect in the Colombian Andes,
    alongside macroclimatic data from Copernicus. Principal Component Analysis (PCA)
    and PERMANOVA identified canopy openness and bushes- and tree-type vegetation
    density as the principal axes of interspecific niche partitioning. The observed
    differences in realized niche breadth were consistent with specialist and generalist
    ecological strategies. A. laevigata was predominantly associated with open-canopy
    areas, warmer micro- and macroclimatic conditions, and narrower edaphic dispersion.
    In contrast, A. cephalotes occupied a wider range of microhabitat conditions.
    This broader realized niche breadth is compatible with previous reports of A.
    cephalotes occurring in urban areas. Together, these findings suggest that niche
    breadth may influence how Neotropical leaf-cutter ants respond to habitat transformation,
    helping to understand the ecological consequences of land-use change.
acknowledgement: I  am profoundly grateful to my parents, María Cristina Castillo
  Sandoval and Víctor Ángel García Aguillón, whose invaluable support made this research
  possible. Their endurance and dedication during the fieldwork were essential for
  the successful collection of the colony samples. Furthermore, our endless discussions
  regarding the natural history and behaviour of these ecosystem engineers deeply
  shaped the conceptualization of this study; this manuscript is a testament to their
  lifelong support of my academic journey. I am also sincerely grateful to my sister,
  Francy Alejandra García Castillo, for generously providing measurement equipment
  essential for our field data collection. I sincerely thank Alejandro Mejía for his
  invaluable local knowledge and field assistance in locating Atta colonies in Grima
  Baja and for providing information that guided us to the sampling area in Choro
  Bajo. I also thank Rosina Soler for her expert professional advice in curating the
  environmental variable matrix during the fieldwork planning phase, as well as for
  her insightful feedback during the elaboration of this manuscript.
article_processing_charge: Yes
article_type: original
author:
- first_name: Diego Fernando
  full_name: Garcia Castillo, Diego Fernando
  id: ae681a14-dc74-11ea-a0a7-c6ef18161701
  last_name: Garcia Castillo
citation:
  ama: 'Garcia Castillo DF. Generalism vs. specialization: Does niche breadth influence
    species responses to anthropogenic land-use change in Neotropical leaf-cutter
    ants? <i>Plos One</i>. 2026;21(10):e0351518. doi:<a href="https://doi.org/10.1371/journal.pone.0351518">10.1371/journal.pone.0351518</a>'
  apa: 'Garcia Castillo, D. F. (2026). Generalism vs. specialization: Does niche breadth
    influence species responses to anthropogenic land-use change in Neotropical leaf-cutter
    ants? <i>Plos One</i>. Public Library of Science. <a href="https://doi.org/10.1371/journal.pone.0351518">https://doi.org/10.1371/journal.pone.0351518</a>'
  chicago: 'Garcia Castillo, Diego Fernando. “Generalism vs. Specialization: Does
    Niche Breadth Influence Species Responses to Anthropogenic Land-Use Change in
    Neotropical Leaf-Cutter Ants?” <i>Plos One</i>. Public Library of Science, 2026.
    <a href="https://doi.org/10.1371/journal.pone.0351518">https://doi.org/10.1371/journal.pone.0351518</a>.'
  ieee: 'D. F. Garcia Castillo, “Generalism vs. specialization: Does niche breadth
    influence species responses to anthropogenic land-use change in Neotropical leaf-cutter
    ants?,” <i>Plos One</i>, vol. 21, no. 10. Public Library of Science, p. e0351518,
    2026.'
  ista: 'Garcia Castillo DF. 2026. Generalism vs. specialization: Does niche breadth
    influence species responses to anthropogenic land-use change in Neotropical leaf-cutter
    ants? Plos One. 21(10), e0351518.'
  mla: 'Garcia Castillo, Diego Fernando. “Generalism vs. Specialization: Does Niche
    Breadth Influence Species Responses to Anthropogenic Land-Use Change in Neotropical
    Leaf-Cutter Ants?” <i>Plos One</i>, vol. 21, no. 10, Public Library of Science,
    2026, p. e0351518, doi:<a href="https://doi.org/10.1371/journal.pone.0351518">10.1371/journal.pone.0351518</a>.'
  short: D.F. Garcia Castillo, Plos One 21 (2026) e0351518.
corr_author: '1'
das_tickbox: '0'
date_created: 2026-10-11T22:02:05Z
date_published: 2026-10-01T00:00:00Z
date_updated: 2026-10-12T11:43:26Z
day: '01'
ddc:
- '570'
department:
- _id: NiBa
doi: 10.1371/journal.pone.0351518
external_id:
  pmid:
  - '42821535'
file:
- access_level: open_access
  checksum: 06ccc9f8806de407b21a168525e324de
  content_type: application/pdf
  creator: dernst
  date_created: 2026-10-12T11:42:06Z
  date_updated: 2026-10-12T11:42:06Z
  file_id: '23109'
  file_name: 2026_PlosOne_GarciaCastillo.pdf
  file_size: 1166607
  relation: main_file
  success: 1
file_date_updated: 2026-10-12T11:42:06Z
fulldoi: https://doi.org/10.1371/journal.pone.0351518
has_accepted_license: '1'
intvolume: '        21'
issue: '10'
language:
- iso: eng
month: '10'
oa: 1
oa_version: Published Version
page: e0351518
pmid: 1
publication: Plos One
publication_identifier:
  eissn:
  - 1932-6203
publication_status: published
publisher: Public Library of Science
quality_controlled: '1'
researchdata_availability: no
scopus_import: '1'
status: public
supplementarymaterial: yes
title: 'Generalism vs. specialization: Does niche breadth influence species responses
  to anthropogenic land-use change in Neotropical leaf-cutter ants?'
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: 21
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
_id: '23089'
abstract:
- lang: eng
  text: The location of the hydrogen-helium (H/He) immiscibility boundary controls
    whether and where helium rain occurs in giant planets, yet it remains uncertain
    because high-pressure experiments are challenging and ab initio simulations are
    limited in system size and simulation time. We map this boundary by computing
    composition-dependent chemical potentials from large-scale molecular dynamics
    driven by machine learning potentials trained on three density functional approximations
    (PBE, vdW-DF, and the hybrid HSE). Across the pressure range of 100-1000 GPa,
    the demixing temperatures are typically  ~ 2000 K lower than previous ab initio
    simulations using small system sizes, and this discrepancy is larger than the
    estimated error from the chosen density functionals, machine learning potentials,
    neglect of nuclear quantum effects, and statistical uncertainties. Fitting the
    H/He mixing free energy to a Redlich-Kister regular solution model rationalizes
    the thermodynamic driving force for phase separation, and provides a predictive
    representation of the boundary. Comparing with current planetary interior profiles
    indicates that helium rain is plausible in Saturn but unlikely in the warmer interior
    of Jupiter. Our results narrow the uncertainty in the H/He immiscibility boundary
    and provide inputs for planetary models that couple demixing, heat transport,
    and composition gradients in gas giants.
acknowledged_ssus:
- _id: ScienComp
acknowledgement: The authors are thankful to Armin Bergermann and Ronald Redmer for
  generously sharing AIMD trajectories and data, and for valuable discussions and
  feedback on the manuscript. The authors also acknowledge the research computing
  facilities provided by the high-performance computing (HPC) cluster at the Institute
  of Science and Technology Austria (ISTA), Berkeley Research Computing (BRC) at the
  University of California, Berkeley (UCB), and Lawrence Livermore National Laboratory
  (LLNL). B.C. was supported by the Laboratory Directed Research and Development (LDRD)
  Program at Lawrence Berkeley National Laboratory (LBNL) under project ID 110990-001.
  Part of this work was performed under the auspices of the U.S. Department of Energy
  by LLNL under Contract DE-AC52-07NA27344. S.H. was supported by the LDRD Program
  at LLNL under project tracking code 23-SI-006.
article_number: '10382'
article_processing_charge: Yes
article_type: original
author:
- first_name: Xiaoyu
  full_name: Wang, Xiaoyu
  id: 8dff9c62-32b0-11ee-9fa8-fc73025e10f3
  last_name: Wang
- first_name: Sebastien
  full_name: Hamel, Sebastien
  last_name: Hamel
- first_name: Bingqing
  full_name: Cheng, Bingqing
  id: cbe3cda4-d82c-11eb-8dc7-8ff94289fcc9
  last_name: Cheng
  orcid: 0000-0002-3584-9632
citation:
  ama: Wang X, Hamel S, Cheng B. Hydrogen-helium immiscibility boundary in gas-giant
    planetary interiors from machine-learning molecular dynamics. <i>Nature Communications</i>.
    2026;17. doi:<a href="https://doi.org/10.1038/s41467-026-77117-8">10.1038/s41467-026-77117-8</a>
  apa: Wang, X., Hamel, S., &#38; Cheng, B. (2026). Hydrogen-helium immiscibility
    boundary in gas-giant planetary interiors from machine-learning molecular dynamics.
    <i>Nature Communications</i>. Springer Nature. <a href="https://doi.org/10.1038/s41467-026-77117-8">https://doi.org/10.1038/s41467-026-77117-8</a>
  chicago: Wang, Xiaoyu, Sebastien Hamel, and Bingqing Cheng. “Hydrogen-Helium Immiscibility
    Boundary in Gas-Giant Planetary Interiors from Machine-Learning Molecular Dynamics.”
    <i>Nature Communications</i>. Springer Nature, 2026. <a href="https://doi.org/10.1038/s41467-026-77117-8">https://doi.org/10.1038/s41467-026-77117-8</a>.
  ieee: X. Wang, S. Hamel, and B. Cheng, “Hydrogen-helium immiscibility boundary in
    gas-giant planetary interiors from machine-learning molecular dynamics,” <i>Nature
    Communications</i>, vol. 17. Springer Nature, 2026.
  ista: Wang X, Hamel S, Cheng B. 2026. Hydrogen-helium immiscibility boundary in
    gas-giant planetary interiors from machine-learning molecular dynamics. Nature
    Communications. 17, 10382.
  mla: Wang, Xiaoyu, et al. “Hydrogen-Helium Immiscibility Boundary in Gas-Giant Planetary
    Interiors from Machine-Learning Molecular Dynamics.” <i>Nature Communications</i>,
    vol. 17, 10382, Springer Nature, 2026, doi:<a href="https://doi.org/10.1038/s41467-026-77117-8">10.1038/s41467-026-77117-8</a>.
  short: X. Wang, S. Hamel, B. Cheng, Nature Communications 17 (2026).
corr_author: '1'
das_tickbox: '1'
dataavailabilitystatement: 'The training data, fitted MLPs, MLP molecular dynamics
  results, and source data underlying all figures and tables in the main text and
  Supplementary Information have been deposited in the Zenodo repository: https://doi.org/10.5281/zenodo.21632034.
  The data-analysis and plotting scripts used to generate the figures and tables in
  the main text and Supplementary Information are available in the GitHub repository:
  https://github.com/ChengUCB/HighPressure_HHe.'
date_created: 2026-10-11T22:02:04Z
date_published: 2026-09-01T00:00:00Z
date_updated: 2026-10-12T11:00:16Z
day: '01'
ddc:
- '540'
department:
- _id: GradSch
- _id: BiCh
doi: 10.1038/s41467-026-77117-8
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  - '42816492'
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title: Hydrogen-helium immiscibility boundary in gas-giant planetary interiors from
  machine-learning molecular dynamics
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  short: CC BY (4.0)
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...
---
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abstract:
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  text: 'Homologous recombination is ubiquitous across evolution, generating variation
    through genetic reshuffling. Although bacteria lack meiotic recombination, homologous
    recombination has been known to extensively shape their genomes. However, the
    mechanisms and ecological conditions sustaining frequent recombination in bacteria
    remain unclear. Using an Escherichia coli–P1 phage model system, we reveal how
    frequent recombination emerges from CRISPR-based herd immunity to a generalized
    transducing phage (DNA vector). Herd immunity maintains phage-susceptible donor
    bacteria, recipient immune bacteria, and transducing phage, which promotes chromosomal
    gene flow that exceeds spontaneous mutation by up to two orders of magnitude.
    Notably, recombination begins as bacterial cultures enter stationary phase, when
    canonical mutation supply through population growth and DNA replication is strongly
    reduced, and recombination can be reinitiated by brief fresh nutrient pulses.
    Genetic analysis showed that stationary-phase recombination requires recA, recB,
    and recG, connecting this process to a defined homologous recombination pathway,
    and suggests a plausible transcriptional regulatory link to transition to nutrient
    limitation. Bacterial herd immunity therefore has an unexpected evolutionary consequence:
    it can promote homologous recombination by turning phages into de facto pollinators.
    This mechanism can help explain how high rates of homologous recombination may
    be sustained across bacterial populations and suggests that bacterial immune systems
    can shape molecular evolution not only by blocking infection but also by regulating
    genetic exchange.'
acknowledgement: We thank Stuart Baird, Nick Barton, Max Joesch, Meriem El Karoui,
  Mato Lagator, Ivana Mašlaňová, Stepan Ovchinnikov, Roman Pantůček, Maroš Pleška,
  Jitka Polechová, and Bryan Wu for their feedback on the manuscript. We are grateful
  to the Redlinger Hut for hosting many discussions about the project away from the
  daily buzz. We acknowledge the core facility CELLIM supported by the Czech-BioImaging
  large RI project (LM2023050 funded by MEYS CR) for their support. This work was
  supported by H2020 European Research Council EVOLHGT No. 648440 to JPB, European
  Commission Programme EXCELES project LX22NPO5103 “National Institute of Virology
  and Bacteriology” to PPl, and a bilateral Czech-Austrian mobility grant 8J3AT003
  funded by MEYS CR and OeAD AT to PPa and CCG.
article_number: msag238
article_processing_charge: Yes
article_type: original
author:
- first_name: Pavel
  full_name: Payne, Pavel
  id: 35F78294-F248-11E8-B48F-1D18A9856A87
  last_name: Payne
  orcid: 0000-0002-2711-9453
- first_name: Pavel
  full_name: Plevka, Pavel
  last_name: Plevka
- first_name: Jonathan P
  full_name: Bollback, Jonathan P
  id: 2C6FA9CC-F248-11E8-B48F-1D18A9856A87
  last_name: Bollback
  orcid: 0000-0002-4624-4612
- first_name: Calin C
  full_name: Guet, Calin C
  id: 47F8433E-F248-11E8-B48F-1D18A9856A87
  last_name: Guet
  orcid: 0000-0001-6220-2052
citation:
  ama: Payne P, Plevka P, Bollback JP, Guet CC. Herd immunity underlies homologous
    recombination in stationary phase bacteria. <i>Molecular Biology and Evolution</i>.
    2026;43(10). doi:<a href="https://doi.org/10.1093/molbev/msag238">10.1093/molbev/msag238</a>
  apa: Payne, P., Plevka, P., Bollback, J. P., &#38; Guet, C. C. (2026). Herd immunity
    underlies homologous recombination in stationary phase bacteria. <i>Molecular
    Biology and Evolution</i>. Oxford University Press. <a href="https://doi.org/10.1093/molbev/msag238">https://doi.org/10.1093/molbev/msag238</a>
  chicago: Payne, Pavel, Pavel Plevka, Jonathan P Bollback, and Calin C Guet. “Herd
    Immunity Underlies Homologous Recombination in Stationary Phase Bacteria.” <i>Molecular
    Biology and Evolution</i>. Oxford University Press, 2026. <a href="https://doi.org/10.1093/molbev/msag238">https://doi.org/10.1093/molbev/msag238</a>.
  ieee: P. Payne, P. Plevka, J. P. Bollback, and C. C. Guet, “Herd immunity underlies
    homologous recombination in stationary phase bacteria,” <i>Molecular Biology and
    Evolution</i>, vol. 43, no. 10. Oxford University Press, 2026.
  ista: Payne P, Plevka P, Bollback JP, Guet CC. 2026. Herd immunity underlies homologous
    recombination in stationary phase bacteria. Molecular Biology and Evolution. 43(10),
    msag238.
  mla: Payne, Pavel, et al. “Herd Immunity Underlies Homologous Recombination in Stationary
    Phase Bacteria.” <i>Molecular Biology and Evolution</i>, vol. 43, no. 10, msag238,
    Oxford University Press, 2026, doi:<a href="https://doi.org/10.1093/molbev/msag238">10.1093/molbev/msag238</a>.
  short: P. Payne, P. Plevka, J.P. Bollback, C.C. Guet, Molecular Biology and Evolution
    43 (2026).
corr_author: '1'
das_tickbox: '1'
dataavailabilitystatement: The data underlying this article are available in the article
  and in its online material.
date_created: 2026-10-11T22:02:04Z
date_published: 2026-10-03T00:00:00Z
date_updated: 2026-10-12T10:51:54Z
day: '03'
ddc:
- '570'
department:
- _id: CaGu
doi: 10.1093/molbev/msag238
external_id:
  pmid:
  - '42827080'
fulldoi: https://doi.org/10.1093/molbev/msag238
has_accepted_license: '1'
intvolume: '        43'
issue: '10'
keyword:
- homologous recombination
- defense systems
- CRISPR-Cas
- herd immunity
- stationary phase
- bacterial evolution
language:
- iso: eng
license: https://creativecommons.org/licenses/by-nc/4.0/
main_file_link:
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  url: https://doi.org/10.1093/molbev/msag238
month: '10'
oa: 1
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pmid: 1
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publication_identifier:
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publication_status: epub_ahead
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title: Herd immunity underlies homologous recombination in stationary phase bacteria
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---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
_id: '23088'
abstract:
- lang: eng
  text: In this review, we provide an engineering assessment of prevalent blood-wetted
    cardiovascular devices, their hematologic complications, and their interconnections
    to identify key areas for future research. In fact, the incidence of cardiovascular
    diseases has promoted the development of various devices to treat these conditions,
    including mechanical circulatory supports (mechanical pumps that assist or replace
    failing hearts), artificial valves to replace faulty heart valves, stents to relieve
    obstructions in blood vessels, vascular grafts to repair/reconstruct damaged vessels,
    patches to reinforce or reconstruct cardiovascular tissues, and other implants.
    The hemocompatibility of these cardiovascular devices, namely their ability to
    interact with blood flow without causing adverse reactions, remains unsatisfactory,
    and recurrent complications include thrombosis, hemolysis, and bleeding. Therefore,
    the discussion provided herein will support readers approaching cardiovascular
    technologies in building a solid foundation and provide everyone with an up-to-date
    overview of ongoing research in this multidisciplinary field.
article_number: '167'
article_processing_charge: Yes
article_type: original
author:
- first_name: Damiano
  full_name: Padovani, Damiano
  last_name: Padovani
- first_name: Nasima S
  full_name: Afsharimani, Nasima S
  id: fe7df522-678a-11eb-9fb9-a37ecf42528e
  last_name: Afsharimani
- first_name: Andrea
  full_name: Cioncolini, Andrea
  last_name: Cioncolini
- first_name: Yu
  full_name: Ding, Yu
  last_name: Ding
citation:
  ama: Padovani D, Afsharimani NS, Cioncolini A, Ding Y. Hematologic complications
    and design challenges in cardiovascular devices. <i>Communications Engineering</i>.
    2026;5. doi:<a href="https://doi.org/10.1038/s44172-026-00771-9">10.1038/s44172-026-00771-9</a>
  apa: Padovani, D., Afsharimani, N. S., Cioncolini, A., &#38; Ding, Y. (2026). Hematologic
    complications and design challenges in cardiovascular devices. <i>Communications
    Engineering</i>. Springer Nature. <a href="https://doi.org/10.1038/s44172-026-00771-9">https://doi.org/10.1038/s44172-026-00771-9</a>
  chicago: Padovani, Damiano, Nasima S Afsharimani, Andrea Cioncolini, and Yu Ding.
    “Hematologic Complications and Design Challenges in Cardiovascular Devices.” <i>Communications
    Engineering</i>. Springer Nature, 2026. <a href="https://doi.org/10.1038/s44172-026-00771-9">https://doi.org/10.1038/s44172-026-00771-9</a>.
  ieee: D. Padovani, N. S. Afsharimani, A. Cioncolini, and Y. Ding, “Hematologic complications
    and design challenges in cardiovascular devices,” <i>Communications Engineering</i>,
    vol. 5. Springer Nature, 2026.
  ista: Padovani D, Afsharimani NS, Cioncolini A, Ding Y. 2026. Hematologic complications
    and design challenges in cardiovascular devices. Communications Engineering. 5,
    167.
  mla: Padovani, Damiano, et al. “Hematologic Complications and Design Challenges
    in Cardiovascular Devices.” <i>Communications Engineering</i>, vol. 5, 167, Springer
    Nature, 2026, doi:<a href="https://doi.org/10.1038/s44172-026-00771-9">10.1038/s44172-026-00771-9</a>.
  short: D. Padovani, N.S. Afsharimani, A. Cioncolini, Y. Ding, Communications Engineering
    5 (2026).
das_tickbox: '0'
date_created: 2026-10-11T22:02:04Z
date_published: 2026-09-30T00:00:00Z
date_updated: 2026-10-12T11:34:48Z
day: '30'
ddc:
- '570'
- '610'
department:
- _id: NanoFab
doi: 10.1038/s44172-026-00771-9
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  - '42816513'
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title: Hematologic complications and design challenges in cardiovascular devices
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...
---
OA_place: publisher
_id: '23072'
abstract:
- lang: eng
  text: "Inferring signal from large quantities of data is one of the most important
    problems in today’s\r\nworld, with neural networks emerging as the most powerful
    solution. While there have been\r\nmassive breakthroughs in the ML space, there
    are two main drawbacks. The first is that\r\nmost of these models are “black boxes”,
    with very little understanding of why they work,\r\nwhich makes it hard to find
    the correct architecture for a given problem. The architecture is\r\ncrucial,
    as the widely used training algorithms are “local” and thus rely on the loss landscape\r\nbeing
    benign enough to find a global optimum. This brings us to the second problem:
    while\r\nthere is a lot of evidence that this can be overcome with large enough
    data, this is less clear\r\nfor datasets which are noisy, do not have enough samples,
    or have a non-standard structure.\r\nHistorically, on a smaller scale, the alternative
    has been simple (Bayesian) statistical methods,\r\nwhich also have the advantage
    of being interpretable and adaptable. However, many of the\r\nclassical results
    cannot be easily extended to the high-dimensional regime in which modern\r\ndata
    lives.\r\nIn this work we want to consider two different settings relating to
    the above. The first is\r\napproximate message passing (AMP), an iterative algorithm
    for high-dimensional (generalized)\r\nlinear models that easily lends itself to
    Bayesian setups, and which in many cases is provably\r\nBayes-optimal. The second
    is an autoencoder with a shallow encoder, for which we can\r\nanalyze the weights
    along the training trajectory of gradient descent. Surprisingly, we will find\r\na
    connection between the two, as we recover certain structures of AMP.\r\nWe will
    first introduce the AMP framework by studying an extension that can be applied\r\nto
    a wider variety of data: rotationally invariant generalized approximate message
    passing\r\n(RI-GAMP). This shows that one can extend the AMP framework to a much
    wider class of\r\nalgorithms, relevant to more practical settings. The results
    are then also confirmed on real\r\ndata that go beyond the theoretical setting.\r\nWe
    then move to the setup of an autoencoder with a shallow encoder and a Bayesian
    prior in\r\nthe high-dimensional regime, in which the input and compression dimensions
    are large and\r\nproportional; this is also a first step towards opening one of
    the black boxes above, as we\r\ncan say precisely when and why the network works.
    While autoencoders are widely used in\r\nmodern ML architectures, most fundamental
    research in this direction has focused on extreme\r\nasymptotic regimes, where
    the autoencoder is either severely over- or under-parameterized,\r\nand which
    do not extend to the proportional high-dimensional regime. We show that for\r\nGaussian
    priors the network finds the global optimum, and these theoretical findings extrapolate\r\nstrikingly
    well to real image data. Next we extend this analysis to more structured priors
    and\r\na deeper decoder. For sparse Gaussian inputs in the training regime studied
    here, the shallow\r\ndecoder does not exploit sparsity and yields the same dynamics
    as in the Gaussian setting.\r\nWe then show how a deeper decoder can break this
    behavior, and interestingly, if we treat the\r\nproblem as an AMP problem, the
    network eventually learns the same decoding as AMP. This\r\ntoo extrapolates to
    real image data.\r\nLastly, we will show that the AMP setup has real practical
    use, by using a practical variant,\r\ngenetic vector approximate message passing
    (gVAMP), for predicting plasma protein levels\r\nfrom genetic information using
    the UKB GWAS data. This is a perfect example of the problems\r\nin the high-dimensional
    regime: approximately 8.4 million dimensions and 40,000 samples,\r\nwhere the
    high noise, low sample count, and large size make it hard for ML methods to work.\r\nTo
    get the optimal prediction accuracy we consider a two-step inference. We first
    consider a\r\npre-processed version of the data, of about 880,000 dimensions,
    on which we run the gVAMP\r\nalgorithm; this allows us to find predictive regions,
    taking into account joint effects between\r\ndifferent regions, and for most proteins
    we end up selecting only about 0.1% of the dimensions.\r\nWe then consider the
    analogue of this small subset, on which we can now run a standard tree\r\nalgorithm
    (XGB) that no longer suffers from the aforementioned problems. This pipeline yields\r\nbetter
    prediction accuracy than recent nonlinear deep learning approaches applied to
    this data,\r\nas we are able to handle the pre-processing in a principled Bayesian
    way."
acknowledged_ssus:
- _id: ScienComp
acknowledgement: "This project was partially supported by the 2019 Lopez-Loreta Prize
  and\r\nthe ERC INF2 project (project number 101161364). Furthermore, the candidate
  acknowledges\r\nthe support from the Scientific Service Units of the Institute of
  Science and Technology Austria\r\nthrough resources provided by Scientific Computing."
alternative_title:
- ISTA Thesis
article_processing_charge: No
author:
- first_name: Kevin
  full_name: Kögler, Kevin
  id: 94ec913c-dc85-11ea-9058-e5051ab2428b
  last_name: Kögler
citation:
  ama: 'Kögler K. Compression and inference in high dimensions: An approximate message
    passing perspective. 2026. doi:<a href="https://doi.org/10.15479/AT-ISTA-23072">10.15479/AT-ISTA-23072</a>'
  apa: 'Kögler, K. (2026). <i>Compression and inference in high dimensions: An approximate
    message passing perspective</i>. Institute of Science and Technology Austria.
    <a href="https://doi.org/10.15479/AT-ISTA-23072">https://doi.org/10.15479/AT-ISTA-23072</a>'
  chicago: 'Kögler, Kevin. “Compression and Inference in High Dimensions: An Approximate
    Message Passing Perspective.” Institute of Science and Technology Austria, 2026.
    <a href="https://doi.org/10.15479/AT-ISTA-23072">https://doi.org/10.15479/AT-ISTA-23072</a>.'
  ieee: 'K. Kögler, “Compression and inference in high dimensions: An approximate
    message passing perspective,” Institute of Science and Technology Austria, 2026.'
  ista: 'Kögler K. 2026. Compression and inference in high dimensions: An approximate
    message passing perspective. Institute of Science and Technology Austria.'
  mla: 'Kögler, Kevin. <i>Compression and Inference in High Dimensions: An Approximate
    Message Passing Perspective</i>. Institute of Science and Technology Austria,
    2026, doi:<a href="https://doi.org/10.15479/AT-ISTA-23072">10.15479/AT-ISTA-23072</a>.'
  short: 'K. Kögler, Compression and Inference in High Dimensions: An Approximate
    Message Passing Perspective, Institute of Science and Technology Austria, 2026.'
corr_author: '1'
date_created: 2026-10-07T11:20:26Z
date_published: 2026-10-08T00:00:00Z
date_updated: 2026-10-12T13:04:49Z
day: '08'
ddc:
- '519'
degree_awarded: PhD
department:
- _id: MaMo
- _id: GradSch
doi: 10.15479/AT-ISTA-23072
doi_confirm: '1'
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file_date_updated: 2026-10-09T13:25:49Z
fulldoi: https://doi.org/10.15479/AT-ISTA-23072
has_accepted_license: '1'
language:
- iso: eng
month: '10'
oa: 1
oa_version: Published Version
page: '222'
project:
- _id: 059876FA-7A3F-11EA-A408-12923DDC885E
  name: Prix Lopez-Loretta 2019 - Marco Mondelli
publication_identifier:
  issn:
  - 2663-337X
publication_status: published
publisher: Institute of Science and Technology Austria
related_material:
  record:
  - id: '14459'
    relation: part_of_dissertation
    status: public
  - id: '12540'
    relation: part_of_dissertation
    status: public
  - id: '17469'
    relation: part_of_dissertation
    status: public
status: public
supervisor:
- first_name: Marco
  full_name: Mondelli, Marco
  id: 27EB676C-8706-11E9-9510-7717E6697425
  last_name: Mondelli
  orcid: 0000-0002-3242-7020
title: 'Compression and inference in high dimensions: An approximate message passing
  perspective'
type: dissertation
user_id: 8b945eb4-e2f2-11eb-945a-df72226e66a9
year: '2026'
...
---
OA_place: publisher
OA_type: hybrid
PlanS_conform: '1'
_id: '23094'
abstract:
- lang: eng
  text: The formation of C(sp2)–heteroatom bonds through cross-coupling catalysis
    is central to the synthesis of pharmaceuticals, agrochemicals and materials. Whereas
    Pd0/PdII catalysis requires substrate-specific ligand optimization to balance
    the competing demands of oxidative addition and reductive elimination, NiI/NiIII
    catalysis offers a complementary strategy because the bond-forming step is intrinsically
    favourable. However, contemporary NiI/NiIII methodologies suffer from insufficient
    oxidative addition reactivity, restricting the aryl halide scope and requiring
    high catalyst loadings. Here we show that mechanistically guided ligand design
    overcomes these limitations. Together with a non-nucleophilic base additive that
    promotes direct visible-light generation of NiI from a bench-stable NiII precatalyst,
    this ligand design enables the coupling of electron-rich aryl bromides with N-,
    O-, S- and P-based nucleophiles at nickel loadings as low as 100 ppm. The method
    is compatible with sterically encumbered nucleophiles and enables gram-scale synthesis
    and late-stage functionalization of complex molecules.
acknowledged_ssus:
- _id: LifeSc
- _id: MassSpec
- _id: NMR
- _id: M-Shop
acknowledgement: We acknowledge ISTA for generous financial support. This research
  was supported by the Scientific Service Units (SSU) of ISTA through resources provided
  by the Lab Support Facility, Mass Spec Facility, NMR facility and the Miba Machine
  Shop. We specifically thank A. Paraskevopoulou for high-resolution mass spectrometry
  measurements. B.P. acknowledges the Austrian Science Fund (PAT 1250924) and the
  ACS GCI Pharmaceutical Roundtable for funding. T.B. thanks the European Union’s
  Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie
  Grant Agreement No. 101034413. D.B. acknowledges funding from the Czech Science
  Foundation (25-17760M). Open access funding provided by Institute of Science and
  Technology (IST Austria).
article_processing_charge: Yes (via OA deal)
article_type: original
author:
- first_name: Aleksander
  full_name: Bena, Aleksander
  id: 4197c39e-e8ec-11ed-86cb-afed934cd664
  last_name: Bena
- first_name: Trisha
  full_name: Banik, Trisha
  id: 506b8e06-c59a-11ee-a1af-ae470719e7d3
  last_name: Banik
- first_name: Christos
  full_name: Giannoudis, Christos
  id: 1bd506c6-e8ec-11ed-86cb-d495f63f2dcd
  last_name: Giannoudis
- first_name: Florian
  full_name: Ortis, Florian
  id: e34c9177-3208-11ee-ac71-a6a15cf2ef29
  last_name: Ortis
  orcid: 0000-0002-0458-5187
- first_name: Daniel
  full_name: Bím, Daniel
  last_name: Bím
- first_name: Haralds
  full_name: Baunis, Haralds
  id: 2eea55ec-e8ec-11ed-86cb-d9c76787acfe
  last_name: Baunis
- first_name: Gayathri
  full_name: Palissery, Gayathri
  id: b02c9d47-50c9-11ef-b52e-b2180bf00ccd
  last_name: Palissery
- first_name: Bartholomäus
  full_name: Pieber, Bartholomäus
  id: 93e5e5b2-0da6-11ed-8a41-af589a024726
  last_name: Pieber
  orcid: 0000-0001-8689-388X
citation:
  ama: Bena A, Banik T, Giannoudis C, et al. Ligand design broadens NiI-catalysed
    C(sp2)–heteroatom couplings of aryl bromides at low catalyst loadings. <i>Nature
    Catalysis</i>. 2026. doi:<a href="https://doi.org/10.1038/s41929-026-01616-6">10.1038/s41929-026-01616-6</a>
  apa: Bena, A., Banik, T., Giannoudis, C., Ortis, F., Bím, D., Baunis, H., … Pieber,
    B. (2026). Ligand design broadens NiI-catalysed C(sp2)–heteroatom couplings of
    aryl bromides at low catalyst loadings. <i>Nature Catalysis</i>. Springer Nature.
    <a href="https://doi.org/10.1038/s41929-026-01616-6">https://doi.org/10.1038/s41929-026-01616-6</a>
  chicago: Bena, Aleksander, Trisha Banik, Christos Giannoudis, Florian Ortis, Daniel
    Bím, Haralds Baunis, Gayathri Palissery, and Bartholomäus Pieber. “Ligand Design
    Broadens NiI-Catalysed C(Sp2)–Heteroatom Couplings of Aryl Bromides at Low Catalyst
    Loadings.” <i>Nature Catalysis</i>. Springer Nature, 2026. <a href="https://doi.org/10.1038/s41929-026-01616-6">https://doi.org/10.1038/s41929-026-01616-6</a>.
  ieee: A. Bena <i>et al.</i>, “Ligand design broadens NiI-catalysed C(sp2)–heteroatom
    couplings of aryl bromides at low catalyst loadings,” <i>Nature Catalysis</i>.
    Springer Nature, 2026.
  ista: Bena A, Banik T, Giannoudis C, Ortis F, Bím D, Baunis H, Palissery G, Pieber
    B. 2026. Ligand design broadens NiI-catalysed C(sp2)–heteroatom couplings of aryl
    bromides at low catalyst loadings. Nature Catalysis.
  mla: Bena, Aleksander, et al. “Ligand Design Broadens NiI-Catalysed C(Sp2)–Heteroatom
    Couplings of Aryl Bromides at Low Catalyst Loadings.” <i>Nature Catalysis</i>,
    Springer Nature, 2026, doi:<a href="https://doi.org/10.1038/s41929-026-01616-6">10.1038/s41929-026-01616-6</a>.
  short: A. Bena, T. Banik, C. Giannoudis, F. Ortis, D. Bím, H. Baunis, G. Palissery,
    B. Pieber, Nature Catalysis (2026).
corr_author: '1'
das_tickbox: '1'
dataavailabilitystatement: All data are available from the authors upon request.
date_created: 2026-10-11T22:02:06Z
date_published: 2026-09-29T00:00:00Z
date_updated: 2026-10-14T06:32:42Z
day: '29'
department:
- _id: BaPi
- _id: GradSch
- _id: RaKl
doi: 10.1038/s41929-026-01616-6
ec_funded: 1
fulldoi: https://doi.org/10.1038/s41929-026-01616-6
language:
- iso: eng
main_file_link:
- open_access: '1'
  url: https://doi.org/10.1038/s41929-026-01616-6
month: '09'
oa: 1
oa_version: Published Version
project:
- _id: 8f1d607d-16d5-11f0-9cad-ab453295ba5e
  grant_number: PAT 1250924
  name: Photoactive ligands for transformative nickel catalysis
- _id: fc2ed2f7-9c52-11eb-aca3-c01059dda49c
  call_identifier: H2020
  grant_number: '101034413'
  name: 'IST-BRIDGE: International postdoctoral program'
publication: Nature Catalysis
publication_identifier:
  eissn:
  - 2520-1158
publication_status: epub_ahead
publisher: Springer Nature
quality_controlled: '1'
researchdata_availability: upon request
scopus_import: '1'
status: public
supplementarymaterial: yes
title: Ligand design broadens NiI-catalysed C(sp2)–heteroatom couplings of aryl bromides
  at low catalyst loadings
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
year: '2026'
...
---
OA_place: repository
OA_type: green
_id: '23095'
abstract:
- lang: eng
  text: "The PXP chain was recently shown to exhibit superdiffusive energy transport
    with Kardar-Parisi-Zhang-like\r\nscaling, z ≈ 3/2, joining a growing number of
    spin chains with this exponent. An understanding of how this\r\nanomalous hydrodynamics
    emerges from microscopics is, however, still lacking. In this work, we show that\r\nfinite-temperature
    energy transport in this model provides a window into the emergence of superdiffusion.
    At\r\nfinite temperature, the energy autocorrelation function exhibits a crossover
    from short-time coherent dynamics to\r\nlong-time hydrodynamics. The short-time
    behavior is dominated by a single magnon band and can be understood\r\nanalytically.
    In momentum space, this regime is characterized by spectral weight near q = π.
    The damping time\r\nτ , which separates the short-time magnon-dominated behavior
    from the late-time hydrodynamics, grows rapidly\r\nupon cooling, consistent with
    an activated form τ (β) ∼ βe\x05β with a gap scale set by the magnon band. At
    longer\r\ntimes, the spectral weight transfers to q = 0 and the running decay
    exponent drifts toward the superdiffusive\r\nvalue z = 3/2. Finite-temperature
    energy transport therefore provides a bridge between microscopic magnon\r\nphysics
    and late-time superdiffusion in the PXP model."
acknowledgement: "We thank M. Serbyn, S. White, and T. Iadecola for insightful discussions.
  Work by T.S. was supported by the U.S.\r\nDepartment of Energy, Office of Science,
  Office of Basic\r\nEnergy Sciences under Early Career Research Program Award\r\nNo.
  DE-SC0025568. T.S. gratefully acknowledges the Institute of Science and Technology
  Austria (ISTA) for hosting\r\nhim during the initial stages of this project. S.J.
  is supported by the U.S. Department of Energy, Office of Science,\r\nBasic Energy
  Sciences, Materials Sciences and Engineering\r\nDivision, under Contract No. DE-AC02-76SF00515.
  M.L.\r\nacknowledges support by the Deutsche Forschungsgemeinschaft (DFG, German
  Research Foundation) under Germany’s\r\nExcellence Strategy—EXC-2111—390814868.
  J.-Y.D. acknowledges funding from the European Union’s Horizon\r\n2020 Research
  and innovation program under the Marie\r\nSkłodowska-Curie Grant Agreement No. 101034413."
article_number: '084306'
article_processing_charge: No
article_type: original
arxiv: 1
author:
- first_name: Jiang
  full_name: Shengtao, Jiang
  last_name: Shengtao
- first_name: Jean-Yves Marc
  full_name: Desaules, Jean-Yves Marc
  id: 6c292945-a610-11ed-9eec-c3be1ad62a80
  last_name: Desaules
  orcid: 0000-0002-3749-6375
- first_name: Marko
  full_name: Ljubotina, Marko
  id: F75EE9BE-5C90-11EA-905D-16643DDC885E
  last_name: Ljubotina
  orcid: 0000-0003-0038-7068
- first_name: Thomas
  full_name: Scaffidi, Thomas
  last_name: Scaffidi
citation:
  ama: Shengtao J, Desaules J-YM, Ljubotina M, Scaffidi T. Finite-temperature crossover
    from coherent magnons to energy superdiffusion in the PXP model. <i>Physical Review
    B</i>. 2026;114(8). doi:<a href="https://doi.org/10.1103/mx9k-1mc6">10.1103/mx9k-1mc6</a>
  apa: Shengtao, J., Desaules, J.-Y. M., Ljubotina, M., &#38; Scaffidi, T. (2026).
    Finite-temperature crossover from coherent magnons to energy superdiffusion in
    the PXP model. <i>Physical Review B</i>. American Physical Society. <a href="https://doi.org/10.1103/mx9k-1mc6">https://doi.org/10.1103/mx9k-1mc6</a>
  chicago: Shengtao, Jiang, Jean-Yves Marc Desaules, Marko Ljubotina, and Thomas Scaffidi.
    “Finite-Temperature Crossover from Coherent Magnons to Energy Superdiffusion in
    the PXP Model.” <i>Physical Review B</i>. American Physical Society, 2026. <a
    href="https://doi.org/10.1103/mx9k-1mc6">https://doi.org/10.1103/mx9k-1mc6</a>.
  ieee: J. Shengtao, J.-Y. M. Desaules, M. Ljubotina, and T. Scaffidi, “Finite-temperature
    crossover from coherent magnons to energy superdiffusion in the PXP model,” <i>Physical
    Review B</i>, vol. 114, no. 8. American Physical Society, 2026.
  ista: Shengtao J, Desaules J-YM, Ljubotina M, Scaffidi T. 2026. Finite-temperature
    crossover from coherent magnons to energy superdiffusion in the PXP model. Physical
    Review B. 114(8), 084306.
  mla: Shengtao, Jiang, et al. “Finite-Temperature Crossover from Coherent Magnons
    to Energy Superdiffusion in the PXP Model.” <i>Physical Review B</i>, vol. 114,
    no. 8, 084306, American Physical Society, 2026, doi:<a href="https://doi.org/10.1103/mx9k-1mc6">10.1103/mx9k-1mc6</a>.
  short: J. Shengtao, J.-Y.M. Desaules, M. Ljubotina, T. Scaffidi, Physical Review
    B 114 (2026).
das_tickbox: '1'
dataavailabilitystatement: "There are no publicly available research data or software\r\nsupporting
  this manuscript. Requests for further information\r\nor data should be sent to the
  authors."
date_created: 2026-10-11T22:02:06Z
date_published: 2026-08-21T00:00:00Z
date_updated: 2026-10-14T05:44:58Z
day: '21'
department:
- _id: MaSe
doi: 10.1103/mx9k-1mc6
ec_funded: 1
external_id:
  arxiv:
  - '2605.19281'
fulldoi: https://doi.org/10.1103/mx9k-1mc6
intvolume: '       114'
issue: '8'
language:
- iso: eng
main_file_link:
- open_access: '1'
  url: https://doi.org/10.48550/arXiv.2605.19281
month: '08'
oa: 1
oa_version: Preprint
project:
- _id: fc2ed2f7-9c52-11eb-aca3-c01059dda49c
  call_identifier: H2020
  grant_number: '101034413'
  name: 'IST-BRIDGE: International postdoctoral program'
publication: Physical Review B
publication_identifier:
  eissn:
  - 2469-9969
  issn:
  - 2469-9950
publication_status: published
publisher: American Physical Society
quality_controlled: '1'
researchdata_availability: upon request
scopus_import: '1'
status: public
supplementarymaterial: yes
title: Finite-temperature crossover from coherent magnons to energy superdiffusion
  in the PXP model
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 114
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '23115'
abstract:
- lang: eng
  text: "We investigate the association between galaxies and neutral O I absorption
    systems at z ∼ 6, which trace metalenriched gas during the epoch of reionization.
    We identify 40 galaxies across six quasar fields, residing in 15\r\noverdensities
    within 300 kpc of the background sight lines. Five O I absorption systems are
    associated with five of\r\nthese overdensities, yielding a covering fraction of\r\n0.27
    0.10\r\n+0.13\r\nwithin 300 kpc. The absorption occurs beyond typical\r\nvirial
    radii, indicating that the gas traces extended overdensity environments rather
    than individual galaxy halos,\r\nunlike the z ∼ 0 circumgalactic medium (CGM),
    which is largely bound to halos. These galaxy-associated\r\nabsorbers account
    for ∼35% of all O I systems seen in blind quasar surveys, implying the remainder
    arise in\r\nlower-mass galaxies below our detection threshold or in dense neutral
    intergalactic medium pockets. The CGM\r\naround these galaxies contains ≳ 2 ×
    106 M⊙ of oxygen, comparable to the interstellar medium oxygen mass of\r\nthe
    galaxies themselves, suggesting that the surrounding environment holds as much
    metal mass as the galaxies.\r\nAll five galaxy-associated systems show significantly
    higher\r\nlog NCII NOI ( / )\r\nratios than absorbers lacking galaxy\r\nassociations.
    Furthermore, relative abundance ratios ([Si/O], [C/O]) reveal that four of the
    five exhibit\r\nenrichment patterns consistent with Population III nucleosynthesis
    at the outskirts of galaxy overdensities. These\r\nrare systems offer a unique
    window into the role of first-generation stars in shaping the early metal enrichment
    of\r\ngalaxies and their environments."
acknowledgement: "IOP Science home\r\nAccessibility Help\r\n\r\nJournals\r\nBooks\r\nPublishing
  Support\r\nLogin\r\nThe Astrophysical Journal\r\nThe American Astronomical Society,
  find out more.\r\n\r\nThe following article isOpen access\r\nEIGER. VIII. First
  Stars Signatures in the Connection between O I Absorption and Galaxies in the Epoch
  of Reionization\r\nJack Higginson, Rongmon Bordoloi, Robert A. Simcoe, Jorryt Matthee,
  Daichi Kashino, Ruari Mackenzie, Ivan Kramarenko, Simon J. Lilly, Anna-Christina
  Eilers, Rohan P. NaiduShow full author list\r\n\r\nPublished 2026 February 24 •
  © 2026. The Author(s). Published by the American Astronomical Society.\r\nThe Astrophysical
  Journal, Volume 999, Number 1\r\nCitation Jack Higginson et al 2026 ApJ 999 49\r\nDOI
  10.3847/1538-4357/ae3e81\r\n\r\nPDFOpens in a new tab.\r\nePub\r\nAuthors\r\nFigures\r\nTables\r\nReferences\r\nArticle
  data\r\nPDFOpens in a new tab.\r\nePub\r\nArticle metrics\r\n626 Total downloads\r\n\r\n22
  total citations on Dimensions.\r\nShare this article\r\nArticle information\r\nAbstract\r\nWe
  investigate the association between galaxies and neutral O i absorption systems
  at z ∼ 6, which trace metal-enriched gas during the epoch of reionization. We identify
  40 galaxies across six quasar fields, residing in 15 overdensities within 300 kpc
  of the background sight lines. Five O i absorption systems are associated with five
  of these overdensities, yielding a covering fraction of \r\n within 300 kpc. The
  absorption occurs beyond typical virial radii, indicating that the gas traces extended
  overdensity environments rather than individual galaxy halos, unlike the z ∼ 0 circumgalactic
  medium (CGM), which is largely bound to halos. These galaxy-associated absorbers
  account for ∼35% of all O i systems seen in blind quasar surveys, implying the remainder
  arise in lower-mass galaxies below our detection threshold or in dense neutral intergalactic
  medium pockets. The CGM around these galaxies contains  ≳  2 × 106 M⊙ of oxygen,
  comparable to the interstellar medium oxygen mass of the galaxies themselves, suggesting
  that the surrounding environment holds as much metal mass as the galaxies. All five
  galaxy-associated systems show significantly higher \r\n ratios than absorbers lacking
  galaxy associations. Furthermore, relative abundance ratios ([Si/O], [C/O]) reveal
  that four of the five exhibit enrichment patterns consistent with Population III
  nucleosynthesis at the outskirts of galaxy overdensities. These rare systems offer
  a unique window into the role of first-generation stars in shaping the early metal
  enrichment of galaxies and their environments.\r\n\r\nExport citation and abstract\r\nBibTeX\r\nRIS\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\nThe
  first generations of stars formed shortly after the Epoch of Recombination within
  dark matter overdensities, producing the first significant quantities of metals
  and enriching the intergalactic medium (IGM) while reionizing hydrogen and helium
  (e.g., R. S. Klessen & S. C. O. Glover 2023). These metals and gas eventually coalesced
  into the first galaxies, which over cosmic time evolved into Milky Way–like systems
  today. Studying these young galaxies and their environments provides critical insight
  into galaxy formation and evolution, constraining models of stellar feedback, gas
  accretion, and chemical enrichment (C.-A. Faucher-Giguère & S. P. Oh 2023; C. Peroux
  & D. Nelson 2024).\r\n\r\nAt low redshift, decades of observations using deep ground-based
  spectroscopy and Hubble Space Telescope (HST) data of background quasars and foreground
  galaxies have built a rich understanding of the circumgalactic medium (CGM) and
  its interplay with galaxies (e.g., J. Tumlinson et al. 2017). The CGM plays a crucial
  role in gas recycling, star formation regulation, and quenching; understanding its
  structure and composition informs galaxy growth models (Y. Peng et al. 2015; E.
  Zinger et al. 2020).\r\n\r\nHigh-redshift studies, leveraging ground- and space-based
  near-infrared (NIR) spectroscopy of quasars, reveal that the early Universe was
  already chemically enriched by the epoch of reionization (e.g., T. J. Cooper et
  al. 2019; L. Christensen et al. 2023; R. L. Davies et al. 2023a). Among tracers
  of neutral and low-ionization gas, O i has emerged as a key probe: surveys report
  an increase in O i number density at z  ≳  5–6 (G. D. Becker et al. 2019; L. Christensen
  et al. 2023; A. M. Sebastian et al. 2024; A. Sodini et al. 2024), while higher-ionization
  species like C iv and Si iv decline, consistent with a softer and evolving UV background
  at the end of reionization (T. J. Cooper et al. 2019; V. D’Odorico et al. 2022;
  R. L. Davies et al. 2023a, 2023b).\r\n\r\nHistorically, connecting absorption systems
  with their host galaxies was challenging due to the difficulty of obtaining deep,
  high-redshift galaxy spectroscopy. This has changed with the advent of JWST, providing
  unprecedented views of early galaxies and their impact on surrounding gas through
  surveys such as EIGER (D. Kashino et al. 2023) and ASPIRE (F. Wang et al. 2023).
  First systematic studies of cool, low-ionization CGM traced by Mg ii around z ∼
  6 galaxies suggest that high-redshift CGM differs significantly from its low-redshift
  counterpart: these galaxies typically have low masses, and strong stellar feedback
  can eject metals far beyond the halo’s gravitational potential (R. Bordoloi et al.
  2024). Such pioneering studies now allow systematic investigations of the CGM in
  the early Universe.\r\n\r\nThe UV background during reionization was inhomogeneous
  and rapidly evolving (e.g., S. R. Furlanetto & S. P. Oh 2005; B. D. Oppenheimer
  et al. 2009; K. Finlator et al. 2013; G. D. Becker et al. 2015; S. E. I. Bosman
  et al. 2022), initially dominated by Population III stars (K. Nakajima & R. Maiolino
  2022; K. Nakajima et al. 2025), then by early star-forming galaxies (L. Jiang et
  al. 2022; J. Matthee et al. 2022), with active galactic nuclei (AGN) contributing
  significantly by z ∼ 5 (A. D’Aloisio et al. 2017; G. Kulkarni et al. 2019; C.-A.
  Faucher-Giguère 2020). Modeling indicates that pockets of Population III star formation
  may persist throughout the Epoch of Reionization (L. Tornatore et al. 2007; R. H.
  Mebane et al. 2018; J. L. Johnson & A. Aykutalp 2019; A. Venditti et al. 2023; O.
  Zier et al. 2025).\r\n\r\nThe large reservoir of neutral O i observed in quasar
  absorption lines at high redshift is typically self-shielded, providing robust estimates
  of chemical abundances. Studying the association of these absorbers with galaxies
  offers unique insight into the CGM of early galaxies, and into potential contributions
  from Population III stars to early chemical enrichment.\r\n\r\nIn this work, we
  study the cool, neutral CGM around galaxies at z ∼ 6, traced by O i absorption from
  the EIGER survey (D. Kashino et al. 2023). We focus on O i absorbers associated
  with [O iii]5008-emitting galaxies at 5.875 <z < 6.378 within 300 kpc of six background
  quasars. We quantify absorber incidence, column densities, and mass estimates, and
  analyze ionic abundances to probe chemical enrichment, including potential contributions
  from Population III stars.\r\n\r\nThis paper is organized as follows. Section 2
  describes the observations; Section 3 details our methods for galaxy selection,
  redshift estimation, galaxy properties, defining galaxy overdensities, absorber
  measurements, and completeness; Section 4 presents the results, including the association
  of O i absorption with galaxies, the incidence of galaxy-associated O i absorbers,
  their chemical abundances, and physical interpretations; Section 5 summarizes our
  conclusions. Throughout, we adopt a ΛCDM cosmology with H0 = 67.66 km s−1 Mpc−1
  (Planck Collaboration et al. 2020).\r\n\r\n2. Observations\r\nEIGER (Program ID
  1243; PI: S. J. Lilly) is a large JWST Wide Field Slitless Spectroscopy (WFSS) program
  totaling 126.5 hr, conducting deep WFSS observations in six extragalactic fields,
  each centered on an ultraluminous quasar at z ≥ 6. These quasars have also been
  observed with deep optical and NIR medium- and high-resolution spectroscopy with
  Magellan/FIRE, Very Large Telescope/X-shooter, and Keck High Resolution Echelle
  Spectrometer (HIRES)/MOSFIRE, providing over 100 hr of complementary NIR spectroscopy
  across the six sight lines. We refer the reader to A.-C. Eilers et al. (2023) and
  A.-C. Ďurovčíková et al. (2025) for data reduction and details of the ground-based
  quasar spectroscopy. In addition, all fields are covered by deep JWST/NIRCam and
  HST imaging. A detailed description of the survey design, methodology, and spectroscopic
  and photometric observation details is provided in D. Kashino et al. (2023), J.
  Matthee et al. (2023), and R. Bordoloi et al. (2024). In this work, we make use
  of the complete EIGER survey of z ≥ 5.9 galaxies spanning all six extragalactic
  fields (D. Kashino et al. 2026).\r\n\r\nWe note that all six quasars were chosen
  with prior knowledge of metal absorption systems along their lines of sight, which
  could in principle bias any attempt to associate galaxies with those absorbers.
  In contrast, a galaxy-centric approach starts with quasar–galaxy pairs without prior
  knowledge of absorption and then builds statistics systematically (see e.g., R.
  Bordoloi et al. 2011; J. K. Werk et al. 2013; R. Bordoloi et al. 2014). However,
  once a blind, well-characterized galaxy survey is in place, the two approaches converge.
  This is conceptually similar to a program that combines quasar spectroscopy performed
  without prior absorber selection with a complete galaxy survey. This work employs
  deep blind galaxy searches in each of the EIGER fields, yielding an emission-line
  complete sample of spectroscopic galaxies (J. Matthee et al. 2022; R. Bordoloi et
  al. 2024) and a complete census of absorption lines along these sight lines (Section
  3.5). By combining these two elements—a galaxy survey with quantified completeness
  and an absorption survey with well-defined sensitivity—we establish a robust framework
  for conducting a census of CGM absorption around galaxies. This combined approach
  has been successfully demonstrated at low redshifts (J. N. Burchett et al. 2019).\r\n\r\n3.
  Methods\r\nIn this section, we describe how galaxy redshifts and properties are
  measured and how absorption lines are identified and measured.\r\n\r\n3.1. Galaxy
  Redshifts\r\nSince our focus is on galaxies at z ∼ 6 near the quasar sight lines,
  we begin with the full EIGER catalog of [O iii] emitters (D. Kashino et al. 2026),
  which contains 948 galaxies detected via [O iii] emission within 5.33 ≤ z ≤ 6.97.
  From this catalog, we select galaxies that (1) lie at least 10,000 km s−1 in the
  foreground of each quasar , (2) are within a projected impact parameter of 300 pkpc,
  and (3) have O i λ1302 coverage in the quasar NIR spectra outside of the Gunn–Peterson
  trough. This yields a sample of 40 galaxies. Of these, 33 fall within the central
  of the EIGER spectroscopic footprint (R. Bordoloi et al. 2024), observed with both
  JWST/NIRCam reverse grism modules (A and B). Because the two modules disperse light
  in opposite directions, they provide independent moderate-resolution (R ∼ 1500)
  spectra of the same target, enabling us to assess redshift measurement uncertainties.\r\n\r\nFollowing
  the procedure in R. Bordoloi et al. (2024), we visually inspect each NIRCam 2D spectrum
  using the custom Python application programming interface (API) zgui(R. Bordoloi
  et al. 2025), extract 1D spectra from each module, and fit Gaussians to the emission
  line to determine redshifts. Redshifts from the two modules are consistent with
  a mean velocity offset of Δv = 9.3 km s−1 with a standard deviation of 24 km s−1
  (Figure 1). We therefore adopt an average redshift uncertainty of ≈24 km s−1 for
  the [O iii] emitters, sufficient for associating metal absorption systems with their
  host galaxies. Hereafter, we focus on this sample of 40 galaxies.\r\n\r\nZoom InZoom
  OutReset image size\r\nFigure 1. Redshift uncertainty distribution of the [O iii]
  emitter EIGER galaxies. The histogram shows the difference in redshift between emission-line
  measurements from NIRCam Grism Module A and Module B spectra, expressed in km s−1.
  Individual redshifts were derived from Gaussian fits to the [O iii] and Hβ lines.
  The two modules yield consistent results with a mean offset and standard deviation
  of Δz = 0.0028 ± 0.0073 (Δv = 9.3 ± 24 km s−1).\r\n\r\nDownload figure:\r\n\r\nStandard
  image\r\nHigh-resolution image\r\n3.2. Galaxy Stellar Mass, Star formation Rate,
  Halo Mass\r\nTo estimate galaxy stellar masses and star formation rates (SFRs),
  we follow the procedure of J. Matthee et al. (2022). We first measure the [O iii]
  and Hβ emission-line fluxes of each galaxy, and combine these with JWST/NIRCam broadband
  photometry (F115W, F200W, and F356W) to perform spectral energy distribution fitting
  at the galaxy redshift using the Prospector code (B. D. Johnson et al. 2021). We
  assume a G. Chabrier (2003) initial mass function (IMF), adopt MIST isochrones (J.
  Choi et al. 2016; A. Dotter 2016), a nonparametric star formation history model
  (R. P. Naidu et al. 2024), and the dust attenuation curve of D. Calzetti et al.
  (2000). Galaxy SFRs are derived by averaging over the most recent 50 Myr of star
  formation history from the Prospector posteriors.\r\n\r\nFigure 2 (left) shows the
  impact parameter distribution of the 40 EIGER galaxies relative to the background
  quasars (black star symbols). The galaxies are randomly distributed with respect
  to the quasar sight lines. The right panel shows their stellar masses and SFRs,
  with symbols color coded by galaxy redshift. Following R. Bordoloi et al. (2024),
  we estimate halo masses and virial radii (Rvir) using abundance matching from P.
  Behroozi et al. (2019). Uncertainties in Rvir are propagated from the 16th and 84th
  percentile stellar mass errors, giving a mean uncertainty of ΔRvir = 1.8 kpc. The
  galaxies span stellar masses of and SFRs of , with all systems being star-forming
  by selection.\r\n\r\nZoom InZoom OutReset image size\r\nFigure 2. Properties of
  40 spectroscopically confirmed galaxies at 5.9 ≤ z ≤ 6.4 within 300 kpc of background
  quasars in the EIGER survey. Each square denotes a galaxy and is color coded by
  redshift. Left: angular positions and impact parameters relative to the background
  quasar (black star), with dashed concentric rings marking 100, 200, and 300 kpc
  at z = 6. Right: stellar mass vs. SFR, averaged over the last 50 Myr. Error bars
  show the 16th–84th percentile uncertainties in stellar mass and SFR.\r\n\r\nDownload
  figure:\r\n\r\nStandard image\r\nHigh-resolution image\r\nOne galaxy (z = 5.910384,
  galaxyID = 15362, qsoID = J159) has an exceptionally high stellar mass of , beyond
  the calibrated range of the P. Behroozi et al. (2019) relation. This object exhibits
  a compact, pointlike morphology and likely hosts an obscured AGN, placing it among
  the recently identified population of little red dots (LRDs; e.g., J. Matthee et
  al. 2024). We do not detect broad Hβ for this object. However, this is not unexpected,
  as LRDs can have Hα/Hβ values as high as ∼10 (M. Brooks et al. (2025; A. Torralba
  et al. 2026, in preparation). As robust AGN modeling at these redshifts is not yet
  established, we estimated its halo mass by linearly extrapolating the P. Behroozi
  et al. (2019) relation from the stable stellar mass regime. We explicitly note where
  this assumption may affect our results in the following sections. Additionally,
  this galaxy has not been plotted in the right panel of 2.\r\n\r\n3.3. Galaxy Overdensities\r\nA
  significant fraction of z ≥ 6 galaxies in the EIGER survey are not isolated but
  are found in overdense environments, either as mergers or members of “protogroups”
  (see, e.g., D. Kashino et al. 2026). The EIGER [O iii] galaxy catalog already merges
  individual [O iii] emission clumps within 2″ into a single system, even when they
  exhibit complex morphologies or merger signatures. To identify larger-scale overdensities,
  we therefore search for galaxies that lie at similar redshifts but are widely separated
  on the sky.\r\n\r\nWithin 300 kpc from the QSO sight lines, we identify overdensities
  around the 40 selected EIGER galaxies using a friends-of-friends algorithm (R. Bordoloi
  et al. 2025). Galaxies are grouped as an overdensity if they lie within 1 pMpc in
  projected separation and within ±1000 km s−1 in redshift space. A galaxy is considered
  part of an overdensity only if all members are “fully” connected, i.e., each galaxy
  in the overdensity satisfies these conditions with all other members. Around each
  detected O i absorption system, we further search for overdensities within ±1500
  km s−1 of the absorber redshift, and merge these associations to ensure all clustered
  galaxies are treated as a single overdensity. This conservative approach ensures
  that we capture the full galaxy environment of O i absorbers. The 40 galaxies studied
  in this work are part of 15 distinct overdensities, with each grouping containing
  1–5 members. The number of galaxies in each grouping is reported in Table 1. The
  typical velocity dispersion of these overdensities is 449.2 km s−1.\r\n\r\nTable
  1. O i Absorption Lines and Associated Galaxy Properties\r\n\r\nLabel\tQuasar\tzgala\tR\t〈v〉b\t#c\tzO
  I\t\t\t\t\t\r\n \t \t \t(kpc)\t(km s−1)\tGalaxies\t \t(cm−2)\t(cm−2)\t(cm−2)\t(cm−2)\t(cm−2)\r\n(1)\t(2)\t(3)\t(4)\t(5)\t(6)\t(7)\t(8)\t(9)\t(10)\t(11)\t(12)\r\na\tJ0100\t5.941\t119.6\t157\t5\t5.945\t\t\t\t\t\r\nb\tJ1148\t6.008\t157.5\t130\t3\t6.011\t\td\t\t\t\r\nc\tJ159\t5.934\t25.2\t−920\t5\t5.913\t\t\t\t⋯\t⋯\r\nd\tJ159\t6.049\t40.8\t230\t2\t6.054\t\t<13.12\t\t⋯\t⋯\r\ne\tJ1030\t6.075\t147.9\t−131\t2\t6.076\te\t\t\t⋯\t⋯\r\nNotes.
  The galaxies listed are the primary members of groups with detections at the lowest
  impact parameter from the host quasar. aRedshift of the primary member of the overdensity.
  bVelocity offset of O i relative to the primary member galaxy of the overdensity.
  cNumber of galaxy members in the overdensity. dFor this system, Si II λ1304 was
  not present, so the value given here is derived from fitting Si II λ1526. eThis
  system is blended; see discussion in Section 3.4.\r\n\r\nDownload table as: \r\nASCII\r\nTypeset
  image\r\n\r\nThroughout this work, we define the galaxy with the smallest impact
  parameter to the background quasar sight line within each galaxy overdensity as
  the primary member. This convention is adopted solely to simplify the presentation
  and does not imply a unique physical association between the intervening absorption
  system and this galaxy. In fact, the concept of a unique absorber–galaxy association
  at high redshift is significantly less robust than in the low-redshift Universe
  (e.g., R. Bordoloi et al. 2024). As discussed in Section 4.1, none of the O i absorption
  systems lie within the virial radius of any individual halo. Even at low redshift,
  the galaxy with the smallest impact parameter is not necessarily the one with the
  smallest velocity offset from the absorber, and therefore does not constitute evidence
  for a unique absorber–galaxy pair (A. Hamanowicz et al. 2020). This behavior is
  also observed for galaxies residing in groups (R. Bordoloi et al. 2011). Our analysis,
  therefore, focuses on the broader environment, which we argue is most appropriately
  characterized by galaxy overdensities, and our choice of a primary galaxy does not
  affect our main conclusions.\r\n\r\n3.4. Absorption-line Detection and Measurements\r\nWe
  follow the procedures outlined in R. Bordoloi et al. (2024) to identify and measure
  the strength of O i absorption systems around EIGER galaxies, and provide a brief
  summary here. We first use a custom Python-based 1D spectrum viewer to identify
  and tabulate all intervening absorption lines in the EIGER quasar spectra. A semiautomated
  CGM absorption-line analysis pipeline is then used to perform the measurements.
  For each galaxy, we extract a ±1500 km s−1 spectral window centered on its systemic
  redshift, for all transitions of interest. In this work, we analyze slices around
  O i λ1302, Si ii λ1260, Si ii λ1304, Si ii λ1527, C ii λ1334, Si iv λ1393, Si iv
  λ1402, C iv λ1548, and C iv λ1550. Each slice is locally continuum-normalized using
  an automated Legendre polynomial fit, with the polynomial order chosen via the Bayesian
  Information Criterion. The continuum fits and absorption features are visually inspected,
  and both rest-frame equivalent widths (Wr) and apparent optical depth (AOD) column
  densities are measured. We define a detection as any absorption system with Wr ≥
  3σw, where σw is the 1σ uncertainty in Wr. We note that this uncertainty contains
  both the statistical uncertainty due to the signal-to-noise ratio of the data and
  the continuum-fitting uncertainty. Nondetections are reported as 2σw upper limits
  measured within ±100 km s−1 of the systemic redshift of the galaxy. For column density,
  we report the 2σ uncertainty on AOD column density as an upper limit on nondetections.
  When a transition is detected in multiple instruments, each spectrum is analyzed
  independently, and the inverse-variance-weighted mean is adopted as the final Wr.
  The details of this automated approach and full documentation of the APIs used can
  be found in R. Bordoloi et al. (2025).\r\n\r\nFor all detections, we perform Voigt
  profile fitting using the rbvfit package, which employs Markov Chain Monte Carlo
  (MCMC) sampling to simultaneously fit multiple absorption systems across different
  instruments (R. Bordoloi & J. Higginson 2025). This approach yields robust column
  densities, resolves the kinematic structure, and enables accurate modeling of blended
  lines. Additionally, since we obtain a marginalized posterior distribution for the
  fitted parameters, the results yield accurate column density estimates even if the
  Doppler b parameter or velocity centroids are not well constrained in moderate-resolution
  spectra (see discussion in R. Bordoloi et al. 2024). In our case, most of the O
  i Si ii C ii transitions are all covered by higher-resolution HIRES spectroscopy
  and thus their properties are well constrained. rbvfit supports two MCMC samplers,
  emcee (D. Foreman-Mackey et al. 2013) and zeus (M. Karamanis et al. 2021; M. Karamanis
  & F. Beutler 2020), both of which are used in this work depending on the complexity
  of the fit. We typically adopt 50 walkers with initial perturbations of either 10−3
  or 10−6, and default chain lengths of 8000–20,000 steps, ensuring the total number
  of steps exceeds 50 times the autocorrelation time. Additional steps are run as
  needed to achieve convergence. In each case, a flat prior is assumed with reasonable
  physical bounds.\r\n\r\nFigure 3 shows an example of Voigt profile fits to O i λ1302
  and Si ii λ1304 lines simultaneously modeled across FIRE, X-shooter, and HIRES.
  We fit a two-component Voigt profile with a mean velocity offset from the host galaxy
  of voffset =  157 km s−1 . This joint fitting maximizes information from all instruments
  while preserving the kinematic detail provided by higher-resolution data. Galaxy
  overdensities associated with this system are marked with green vertical ticks.
  This system has a total O i column density 13.46. All other O i fits are presented
  in Figure 8. All absorption-line measurements are presented in Table 1.\r\n\r\nZoom
  InZoom OutReset image size\r\nFigure 3. Voigt profile fits to O i and Si ii absorption
  profiles at z = 5.945 toward the quasar SDSS J0100+2802. Shown are the flux (black),
  error spectrum (red), best-fit Voigt model (orange/black), and individual Voigt
  components (thin blue), using data from FIRE, X-shooter, and HIRES. Vertical green
  lines mark galaxy members of the associated overdensity. Spectra from all instruments
  and all transitions are simultaneously fit using the rbvfit Bayesian absorption-line
  fitter.\r\n\r\nDownload figure:\r\n\r\nStandard image\r\nHigh-resolution image\r\nWe
  note that an O i and Si ii absorption system is detected along the J1030 quasar
  sight line at z ∼ 6.075, blended with an intervening C iv absorber at z ∼ 4.948
  (Figure 8, top left panels; see also C. G. Díaz et al. 2021). The z ∼ 6.076 system
  is confirmed by the independent detection of Si ii, Mg ii, C ii, and Fe ii absorption
  in FIRE and X-shooter data, and we simultaneously fit the C iv, O i, and Si ii systems
  across three instruments. Although the proximity of the C iv doublet in wavelength
  space introduces an inherent degeneracy with the O i and Si ii pair, high-resolution
  HIRES data reveal sufficient kinematic substructure to warrant an additional component
  at a mean velocity offset of voffset = –85.4 km s−1. We interpret this component
  as O i, supported by the aforementioned coincident detections. To constrain the
  system, we use the secondary lines to fix the velocity centroid of the O i component
  and perform simultaneous Voigt profile fitting across all three instruments, including
  both C iv transitions and single-component O i and Si ii models. The column density
  reported in this work corresponds to this singular O i component, and the system
  is marked with an asterisk in Table 1.\r\n\r\n3.5. O i Absorption Detection Completeness\r\nWe
  quantify the completeness of O i absorption detection around each galaxy as follows.
  For each galaxy overdensity, we compute the detection sensitivity on a pixel-by-pixel
  basis following the general framework of, e.g., K. M. Lanzetta et al. (1987), M.
  L. Bernet et al. (2010), and N. L. Mathes et al. (2017). In particular, we use a
  continuum-normalized spectral slice of ±1500 km s−1 centered on the expected O i
  absorption at the redshift of each galaxy overdensity.\r\n\r\nWe define the completeness
  in O i absorption detection in a single instrument as\r\n\r\nwhere H is the Heaviside
  step function, and is the equivalent-width cutoff at which completeness is defined.
  We adopt Å to facilitate comparison with the literature (see Section 4.2). Nσ is
  the detection threshold, which we set to Nσ = 3 by convention. The equivalent-width
  error, σEW(z), is given by\r\n\r\nwhere Δλj is the wavelength spacing between adjacent
  pixels (set by the spectrograph), and npix is the number of pixels over which the
  equivalent width is computed. We adopt the typical width of an O i absorber as npix
  for our analysis, yielding npix, X-shooter = 10, npix, HIRES = 50, and npix, FIRE
  = 11, respectively. This is a conservative approach to calculating completeness,
  as the typical width of the absorbers is larger than the resolving power of the
  instruments. We neglect continuum-fitting errors, so σEW(z) reflects only statistical
  uncertainties from the spectra. Any chip gaps or sky lines are masked. σI and Ic
  are the flux uncertainty and continuum levels of the spectrum.\r\n\r\nFor galaxy
  overdensities observed with multiple spectrographs, we define the combined completeness
  as requiring detection in at least one instrument across the relevant wavelength
  range. For example, with three or more instruments available,\r\n\r\nwhere the logical
  OR (∨) runs over all instruments i ∈ X-shooter, FIRE, HIRES. We then compute the
  mean completeness for each overdensity, and obtain the overall mean completeness,
  , by averaging over all overdensities weighted by their wavelength coverage. This
  yields a mean completeness of 91.4% for O i absorption around galaxy overdensities
  in the EIGER survey for 0.05 Å.\r\n\r\n4. Results\r\nIn this section, we present
  the variation of O i absorption around z ∼ 6 galaxies, the incidence of O i absorption
  per comoving path length that is due to O i absorption around galaxies, and the
  chemical abundance of these systems.\r\n\r\n4.1. Variation of O i Absorption around
  Galaxies\r\nSince all 40 galaxies in our sample reside within 15 identified overdensities
  (Section 3.3), we investigate whether O i absorption is preferentially detected
  in these environments. For clarity, we show the primary galaxy in each overdensity
  (as defined in Section 3.3) when presenting the radial distribution of O i absorption.
  Out of the 15 overdensities, 5 show associated O i absorption.\r\n\r\nFigure 4 shows
  the 2D spatial distribution of galaxies around these five detected systems, with
  the size depicting the virial radii of the galaxies. The galaxies are randomly distributed
  around the absorbers, and we do not find correlations with stellar mass, star formation,
  or other galaxy properties. In all five cases where we have O i detection, the galaxy
  member with the minimum impact parameter is also the member with the lowest R/Rvir.\r\n\r\nZoom
  InZoom OutReset image size\r\nFigure 4. Galaxy overdensities around z ∼ 6 O i absorbers
  in the EIGER survey. Each panel shows the background quasar (red star) at the center,
  with foreground galaxies associated with O i absorption marked as circles. Circles
  are color coded by the velocity offset between the galaxy and the O i absorber,
  and circle sizes are scaled to their virial radii. Only galaxies within 300 kpc
  of the quasar are shown, highlighting the overdensities nearest the absorbers. Dashed
  circles denote projected impact parameters of 50, 100, 200, and 300 pkpc from the
  quasar.\r\n\r\nDownload figure:\r\n\r\nStandard image\r\nHigh-resolution image\r\nFigure
  5 presents 1D the radial profiles around the primary galaxies in these systems.
  The marker size indicates the number of member galaxies in each overdensity, while
  the color encodes the velocity offset from the corresponding O i absorption. Panels
  (a) and (c) show impact parameter (R), and panels (b) and (d) show the same distribution
  normalized by the halo virial radius (R/Rvir).\r\n\r\nZoom InZoom OutReset image
  size\r\nFigure 5. Radial absorption profiles of O i absorption at z ∼ 6. Each point
  marks the impact parameter to the nearest galaxy in a galaxy overdensity, with all
  detected O i absorption arising in such environments. Overdensities with O i absorption
  are shown as circles, while nondetections (2σ limits) are indicated by downward
  arrows. Points are color coded by the velocity offset between the galaxy redshift
  and the O i absorber, and their size scales with the number of members in the overdensity.
  The mean uncertainty on the virial radius is ΔRvir = 1.81 kpc. Top panels: rest-frame
  equivalent width vs. impact parameter (R, left) and normalized impact parameter
  (R/Rvir, right). Bottom panels: same as above, but for O i column densities.\r\n\r\nDownload
  figure:\r\n\r\nStandard image\r\nHigh-resolution image\r\nMost of the O i detections
  occur within R ≲ 175 kpc of the primary galaxy, corresponding to an incidence rate
  of , estimated using 68% Wilson score confidence intervals. Within 100 kpc, the
  incidence is , increasing to for R ≤ 50 kpc. Conversely, at R  >  150 kpc, an incidence
  of is measured. Within 300 kpc of the primary galaxy, the overall incidence is ,
  with values of for 50 ≤ R ≤ 300 kpc and for 100 ≤ R ≤ 300 kpc. These rates are substantially
  weaker than the incidence of strong Mg ii absorption at z ∼ 6 (R. Bordoloi et al.
  2024), indicating that neutral oxygen preferentially traces a different phase of
  the circumgalactic environment.\r\n\r\nPanels (b) and (d) reveal that O i absorbers
  are typically located at much larger R/Rvir than strong low-ionization tracers such
  as Mg ii. This distinction suggests that O i absorption at z ∼ 6 is not confined
  to the CGM of an individual galaxy but instead reflects the larger-scale gaseous
  environment of galaxy overdensities—what might be described as “cosmic ecosystems”
  rather than isolated halos.\r\n\r\nComparing the stellar mass distributions of overdensities
  with and without O i absorption, we find no statistically significant differences.
  The mean stellar mass of galaxies in overdensities with absorption is , compared
  to for those without.\r\n\r\nWe emphasize that at z ∼ 6, the large R/Rvir values
  of these halos imply that O i absorption typically arises at scales well beyond
  the typical CGM [R/Rvir ≲ 1] (J. Tumlinson et al. 2017) probed by low-ionization
  lines at lower redshift. Unlike the low-z CGM, where metal absorbers are closely
  tied to the halo of a single massive galaxy, the O i absorbers studied here appear
  to be linked to extended networks of low-mass, young galaxies embedded in shared
  overdensities. Over cosmic time, these small systems and their diffuse gaseous environments
  are expected to merge and evolve into more massive systems, eventually forming Milky
  Way–like galaxies by z = 0. Thus, neutral O i at reionization is best understood
  not as a tracer of isolated galactic halos, but as a probe of the extended environments
  that connect galaxies, gas, and structure growth in the early Universe.\r\n\r\nBecause
  O i absorption traces dense, neutral gas and requires only minimal ionization corrections,
  we can place a conservative lower limit on the total oxygen mass associated with
  the EIGER galaxies. These estimates are intended as simple, order-of-magnitude calculations
  to provide intuition about the amount of neutral oxygen relative to the observed
  galaxy properties. Following the formalism of R. Bordoloi et al. (2014), the oxygen
  mass contained in an annulus bounded by Rin and Rout is\r\n\r\nwhere Rin and Rout
  are the inner and outer radii of the annulus, fc is the covering fraction (the incidence
  of O i detections in that bin), 〈NOI〉 is the mean O i column density in the annulus,
  and mO = 16 mp is the mass of an oxygen atom, with mp being the mass of a proton.
  For a conservative lower limit, we adopt fion = 1, where fion is the ionization
  fraction (i.e., we assume that all of the oxygen mass is in the neutral phase).
  We justify this assumption as follows: O i is tightly coupled to H i through charge
  exchange, and in dense gas, the required ionization correction is minor, even under
  strong radiation fields such as the Fermi Bubbles (R. Bordoloi et al. 2017; T. Ashley
  et al. 2022). Under a typical metagalactic UV background, it is generally less than
  10% and does not significantly alter the inferred oxygen abundance. In addition,
  oxygen does not deplete onto dust grains, unlike Si or C. For these reasons, we
  consider the approximation NO,total ≈ NOI to be valid for our analysis.\r\n\r\nWe
  compute masses in two radial bins: 0–100 kpc and 100–300 kpc, respectively. The
  total oxygen mass within radius is obtained by summing the masses of the constituent
  annuli. This yields a strict lower limit of  ≳  2 ×106M⊙ on the total oxygen mass
  within = 300 kpc.\r\n\r\nWe compare the inferred oxygen mass in the extended environment
  of our sample with the total oxygen content in the interstellar medium (ISM) of
  a typical z ∼ 6 galaxy. In computing this quantity, we make the following assumptions.
  First, we assume that all galaxies in this work lie on the typical z ∼ 6 mass–metallicity
  relation, derived by stacking [O iii] emitter galaxies (J. Matthee et al. 2022),
  and we adopt the gas-phase metallicity from this relation for each galaxy.\r\n\r\nBecause
  direct measurements of the total H2 and H i gas content are not available at these
  redshifts, we extrapolate the molecular gas fraction from L. J. Tacconi et al. (2018)
  to z ∼ 6 and adopt a conservative H i gas fraction based on local observations (S.
  Huang et al. 2012). We note that high-z galaxies are likely more gas-rich than their
  local counterparts; therefore, the inferred ISM gas masses should be considered
  lower limits.\r\n\r\nWith these caveats in mind, we estimate the total ISM oxygen
  mass as\r\n\r\nwhere we define . Here, XO is the gas-phase oxygen abundance derived
  from the mass–metallicity relation, and and MHI are the molecular and atomic gas
  masses derived as described above. For our galaxy sample, the mean stellar mass
  is , corresponding to an ISM oxygen mass of MO,ISM  ≳  6.8 × 105 M⊙. Remarkably,
  this indicates that the typical ISM oxygen content is comparable to the oxygen mass
  in the extended environment around these galaxies, implying that the circumgalactic
  or intergalactic medium at z ∼ 6 contains a substantial reservoir of oxygen. While
  these estimates depend on several specific assumptions, the inferred ISM and CGM
  oxygen masses appear to be of similar magnitude.\r\n\r\nAt low redshift, both L*
  and sub-L* galaxies similarly exhibit substantial metal content in their circumgalactic
  medium (CGM), with the CGM containing at least as much metal as the ISM of their
  host galaxies (J. Tumlinson et al. 2011; R. Bordoloi et al. 2014). A key difference
  is that, whereas the low-z CGM is typically gravitationally bound to its host galaxy,
  at high redshift much of the gas exists in the extended environment of galaxy overdensities
  rather than being bound to individual galaxies (see also R. Bordoloi et al. 2024).\r\n\r\n4.2.
  Expected Incidence of O i Absorbers\r\nIn this section, we report the expected redshift-path
  incidence of O i absorbers around [O iii] emitting galaxies detected in the EIGER
  survey. We define the number of O i absorbers associated with each galaxy overdensity
  per unit absorption distance above a detection threshold (WOI ≥ 0.05Å ) as\r\n\r\n\r\nHere,
  Rmax = 300 kpc is the survey radius adopted in this work, and is the mean O i absorber
  detection completeness (see Section 3.5; 91.4% for WOI ≥ 0.05 Å). nOD is defined
  as\r\n\r\n\r\nngal is the number density of [O iii] emitting galaxies per unit comoving
  volume, estimated from the [O iii] luminosity function at z ∼ 6. And 〈overdensity
  size〉 is simply the mean number of galaxies in each galaxy overdensity empirically
  measured to be 〈overdensity size〉 = 2.67. fc is the O i absorption covering fraction
  within 300 kpc for WOI ≥ 0.05 Å (). (The covering fraction within 300 kpc is independent
  of the definition of the primary member.)\r\n\r\nTo estimate the number density
  of galaxies per unit comoving volume (ngal), we integrate the z ∼ 6 [O iii] luminosity
  function derived from the EIGER survey, with a minimum luminosity of Lmin = 1042.2
  ergs−1 (J. Matthee et al. 2022):\r\n\r\n\r\nwhere Φ(L) is the [O iii] luminosity
  function defined as\r\n\r\n\r\nHere, Φ* is the characteristic number density, L*
  is the characteristic luminosity, and α is the faint-end slope. We adopt Φ* = 10−4.02
  Mpc−3, L* = 1043.33 ergs−1, and α = −1.92, values derived from detailed completeness
  calculations of the EIGER [O iii]-emitting galaxies (R. Mackenzie et al. 2026, in
  preparation). This results in ngal = 8.586 × 10−04 Mpc−3. Using these values in
  Equation (6) yields , for O i absorption around galaxies at a mean galaxy redshift
  of 6.001.\r\n\r\nAll calculations in this section are performed with a detection
  threshold of WOI > 0.05Å, since the survey is highly complete down to this equivalent-width
  limit and because most of the literature surveys we compare against adopt the same
  threshold.\r\n\r\nWe emphasize that this approach differs from blind QSO absorption-line
  surveys (e.g., G. D. Becker et al. 2006; L. Christensen et al. 2023; A. M. Sebastian
  et al. 2024; A. Sodini et al. 2024), where all O i absorption-line systems along
  the full quasar redshift path are counted to compute dN/dX directly, under the assumption
  that the absorber cross section is contributed by all galaxies. In contrast, our
  method begins by defining the absorber cross section around galaxy overdensities
  and then estimating the corresponding contribution to dN/dX from the galaxy overdensities
  under study. Comparing these two approaches constrains the fraction of O i (or other
  metal) absorption systems that arise in the extended halos of these galaxies. Figure
  6 shows these literature measurements as colored circles, while the contribution
  to dN/dX around z ∼ 6 galaxy overdensities is indicated by an orange square. To
  quantify the relative contribution of galaxy overdensities, we fit a single power
  law to all literature values at z  >  4 (blue dashed line with shaded region). Comparing
  the dN/dX inferred from quasar absorption-line surveys at z ∼ 6 to our measured
  value, we find that O i dN/dX around z ∼ 6 EIGER galaxy environments account for
  35% ± 16% of all O i absorption-line systems detected in blind quasar surveys. This
  implies that [O iii] emitting galaxy environments at z ∼ 6 contribute roughly one-third
  of the O i absorption systems at that epoch. Although the EIGER QSOs were selected
  to have known absorption systems along their sight lines, the EIGER galaxy survey
  around these sight lines is highly complete and independent of this selection. Therefore,
  we can create an unbiased measurement of the absorption cross section (dN/dX) around
  these galaxy overdensities. We justify this comparison to blind absorption surveys
  in Section 2.\r\n\r\nZoom InZoom OutReset image size\r\nFigure 6. Incidence of O
  i absorbers per comoving path length, dN/dX. Values are derived from all O i absorption
  lines along high-z quasar sight lines. Literature measurements are shown from G.
  D. Becker et al. (2019; blue circles), L. Christensen et al. (2023; purple circles),
  and A. M. Sebastian et al. (2024; red circles). The blue dashed line shows a power-law
  fit to the z  > 4 literature data, with the shaded region marking the 1σ uncertainty.
  The orange square gives the inferred dN/dX when including only O i absorption associated
  with host galaxies (see Section 4.2), indicating that only ∼35% of O i absorbers
  at z ∼ 6 arise in galaxy environments.\r\n\r\nDownload figure:\r\n\r\nStandard image\r\nHigh-resolution
  image\r\nThis in turn suggests that ∼65% of the O i absorption systems detected
  along quasar sight lines at the epoch of reionization are not associated with [O
  iii] emitter galaxy overdensities. Either the bulk of O i absorption resides in
  isolated pockets of neutral IGM gas outside extended galaxy halos, or it is contributed
  by even lower-luminosity, less massive galaxies () that fall below the EIGER detection
  limits. Such systems may also be detected in galaxy halos that are oxygen-poor or
  lack strong [O iii] emission features, since our galaxy identifications primarily
  rely on [O iii] and Hβ emission lines.\r\n\r\nSimulations suggest that O i absorption
  should primarily arise in galactic halos rather than in the diffuse IGM, since metals
  are not widely distributed and ionization fronts propagate more quickly than metals
  (B. D. Oppenheimer et al. 2009; K. Finlator et al. 2013). Very low-mass protogalaxies
  forming their first stars may blur the boundary between IGM and CGM, enriching their
  surroundings with metals, especially if their star formation is bursty and prolific.
  If sufficiently numerous, such systems could contribute a nonnegligible fraction
  of oxygen in the early Universe.\r\n\r\nRecent observations support this possibility.
  K. Nakajima et al. (2025) reported a strongly lensed (μ = 98) galaxy at z ≈ 6.6
  with a stellar mass upper limit of only ∼2700 M⊙ and a dynamical mass ∼100 times
  larger. The source shows emission and may be dominated by Population III stars.
  This provides direct evidence of oxygen production in extremely low-mass systems.
  A population of such ultralow-mass dwarf galaxies could plausibly account for the
  ∼65% of O i absorbers detected along quasar sight lines that are not associated
  with galaxies in our survey. Our sensitivity limit of (J. Matthee et al. 2022) means
  such dwarfs remain undetected. However, these galaxies may lack a dense enough CGM
  to shield neutral O i from the UV background; thus, even if they produce oxygen,
  neutral O i may not survive (K. Finlator et al. 2013). Interestingly, simulations
  by S. Kušmić et al. (2024) showed that the contribution of metal ions, including
  O i, is only weakly correlated with the stellar mass of the galaxy, and the contribution
  is indistinguishable when comparing across galaxy luminosities. Additionally, they
  argue that due to the steep slope of the stellar mass function, lower-mass, lower-luminosity
  galaxies contribute the majority of absorbing metal ions in the CGM and IGM.\r\n\r\nLater
  simulation works by C. Doughty et al. (2018); C. Doughty & K. Finlator (2019) suggest
  that as the Epoch of Reionization continues, O i will reduce overall but be preferentially
  found in higher column density regions close to halos, as they have a better ability
  to self-shield from ionizing photons. In fact, C. Doughty & K. Finlator (2019) found
  that at z = 6 the majority of O i mass was located in the ISM of galaxies and only
  ∼30% of O i mass was found in the CGM and IGM. In contrast, in this work, we find
  that a substantial (comparable to ISM mass) oxygen mass exists outside galaxies;
  however, we stress that our mass measurements are order-of-magnitude estimates.
  A more direct comparison between these simulations and this work is the covering
  fraction. They report ∼5%–25% covering fraction at z = 6 for O i with out to 102
  pkpc. In the EIGER survey, we report a covering fraction using a minimum threshold
  of WOI ≥ 0.05 Å (or approximately logNOI > 13.7 cm−2) out to 300 kpc. Given the
  large measurement uncertainties and different definitions of associated galaxies,
  the covering fractions are qualitatively consistent between the two works.\r\n\r\nThe
  simulations of K. Finlator et al. (2013) suggest that O i absorbers with are most
  likely associated with halos of mass ∼109 M⊙, where self-shielding is efficient.
  They further predict that only ∼13% of all O i absorption systems should reside
  in halos of 1010–1011.5 M⊙, the mass range of galaxies probed in this work. By contrast,
  we measure a higher dN/dX of ∼35%, but qualitatively our results remain consistent
  with the idea that roughly two-thirds of O i absorbers are associated with undetected
  ∼109 M⊙ halos. Future observations targeting lower-luminosity galaxies and higher
  redshifts will be essential to test these predictions.\r\n\r\nAfter the initial
  posting of this manuscript, G. Pruto et al. (2026) presented a simulation-based
  study that adopts the observational compilation shown in Figure 6 as a reference
  and explores the corresponding behavior in numerical models. Our minimum Wr threshold
  corresponds to ; therefore, the most appropriate comparison is with their sample.
  Qualitatively, the two sets of results are in agreement. A key distinction lies
  in the definition of galactic environment. We characterize environments in terms
  of galaxy overdensities, which we argue is the most appropriate description of where
  O i absorbers reside at z ≈ 6, whereas G. Pruto et al. (2026) define the CGM based
  on the virial radii of halos with . As a result, a direct quantitative comparison
  is not straightforward. Nevertheless, their inferred dN/dX corresponds to an incidence
  rate of O i absorbers of ∼58% ± 11%, which is consistent with our measurements within
  the uncertainties. This agreement may depend on their tighter constraints on absorber
  location and on the adopted minimum Wr or threshold. G. Pruto et al. (2026) further
  report that ∼80% of O i absorbers with are predicted to lie outside the CGM, also
  in qualitative agreement with our findings.\r\n\r\n4.3. Metal Abundances in O i
  absorber population\r\nIn this section, we examine the relative abundances and metal
  column density ratios of O i absorbers associated with galaxy overdensities, and
  compare them to O i absorbers without any associated galaxies. To enable a fair
  comparison, we restrict our analysis to the six quasar sight lines from the EIGER
  survey and identify all O i absorption systems in the redshift range where an [O
  iii]-emitting galaxy could be detected (5.9 ≤ zOI ≤ zQSO). We detect 10 O i absorption
  systems in total, 5 of which have associated galaxy overdensities (Table 1) and
  5 are without any identified galaxy association.\r\n\r\nWe first compare the ionic
  column density ratios in these two populations. Figure 7 (top panels) shows the
  ratios of NSiII/NOI and NCII/NOI as functions of NOI. Systems located near galaxy
  overdensities (blue squares) systematically show higher Si ii/O i and C ii/O i ratios
  compared to systems without associated overdensities (green crosses). This offset
  could reflect differences in metallicity, or alternatively, the effects of ionization.
  However, since the majority of these O i systems lack detectable high-ionization
  transitions, it is reasonable to assume that neutral oxygen and singly ionized silicon
  and carbon dominate the elemental reservoirs (see also L. Christensen et al. 2023).
  In those cases, the observed ionic ratios provide direct tracers of relative abundances.
  Two exceptions are found along the J0100 and J1148 sight lines, which do exhibit
  Si iv and C iv absorption; for these systems, the degeneracy between chemical composition
  and ionization corrections cannot be resolved. It is plausible that, on average,
  O i absorption found near galaxy overdensities has higher elemental abundance ratios
  as the non-galaxy-associated absorbers either have significantly lower-luminosity
  and less massive galaxies, which would be expected to produce less metal, or there
  are truly no galaxies associated with this population.\r\n\r\nZoom InZoom OutReset
  image size\r\nFigure 7. Top panels: ion column density ratios of Si ii to O i (left)
  and C ii to O i (right) as a function of the detected O i column densities, shown
  in logarithmic units. Absorbers associated with galaxy overdensities (blue squares)
  and those not associated with galaxy overdensities (green crosses) exhibit clear
  variations in their column density ratios. One sight line with no detected Si ii
  absorption is indicated with a downward arrow, where a 2σ upper limit on the column
  density is assumed. Bottom panel: relative abundance ratios [Si/O] vs. [C/O] with
  respect to solar abundance. The background contours show the IMF-weighted abundance
  distributions from Population II and Population III SN models. Orange and pink circles
  indicate abundance ratios predicted by low-metallicity Population II SN models.
  The abundance ratios of several O i absorbers associated with galaxy overdensities
  are consistent with a significant contribution from Population III SNe.\r\n\r\nDownload
  figure:\r\n\r\nStandard image\r\nHigh-resolution image\r\nWe next compute the relative
  abundances [Si/O] and [C/O], presented in the bottom panel of Figure 7. These abundances
  are defined as\r\n\r\n\r\nwhere NSi,tot and NC,tot represent the summed ionic column
  densities. For systems with detected high-ionization absorption (C iv or Si iv),
  we include both low- and high-ionization states (NSiII + NSiIV and NCII + NCIV),
  marking these measurements as lower limits (blue upward arrows in the figure) since
  additional undetected ionization states may be present. We note that in the two
  systems (a and b) exhibiting high-ionization absorption (see Table 1), the low-
  and high-ionization absorption components are offset in velocity by Δv = –66 km
  s−1 and –69 km s−1, respectively. These offsets are within ≲1.5 resolution elements
  of the instrument, and therefore we cannot statistically distinguish whether the
  low- and high-ionization components are kinematically distinct. This is suggestive
  of a complex, potentially multiphase gaseous environment in the outskirts of these
  galaxies. For systems without detected high-ionization transitions, we adopt NSiII
  and NCII as the dominant contributions. We assume NO,tot ≈ NOI, as ionization corrections
  for O i are typically very small at high O i column densities (see Section 4.1 for
  discussion). We adopt solar reference abundances of = −1.18 ± 0.05 and (M. Asplund
  et al. 2021).\r\n\r\nFigure 7 (bottom panel) reveals a striking separation between
  O i absorbers associated with galaxy overdensities (blue squares) and those without
  galaxy associations (green crosses). Systems near galaxies are found in the upper
  left of the [Si/O]–[C/O] diagram, with two cases exhibiting high-ionization absorption
  (lower abundance limits, blue arrows), which will offset them even farther from
  the locus of nongalaxy absorbers.\r\n\r\nWe place these abundance patterns in the
  context of chemical enrichment models from different stellar populations (see also
  L. Christensen et al. 2023). The contours and colored circles in Figure 7 highlight
  predicted [C/O] and [Si/O] yields from representative Population II and Population
  III supernova (SN) models, weighted by a Salpeter IMF. The weighting by number of
  stars predicted by an IMF is done to represent the typical observational relative
  abundance distribution in these models. These are not exhaustive but span the dominant
  theoretical expectations.\r\n\r\nPopulation III pair-instability SNe (PISNe; 140–260M⊙;
  light green contours) predict narrow [C/O] ≃ –0.7 and high [Si/O] values, inconsistent
  with any of our observed systems. Such PISNe are also expected to produce substantial
  amounts of iron-peak elements, leading to elevated Fe/O ratios (J. Tumlinson et
  al. 2004). We will investigate Mg ii and Fe ii absorption associated with z ∼ 6
  galaxies in an upcoming work (J. Higginson et al. 2026, in preparation). Models
  of massive Population III stars (10–100 M⊙) produce both hypernovae (gray contours;
  E > 1052 erg) and standard core-collapse SNe (light blue contours; A. Heger & S.
  E. Woosley 2010), spanning a broader region overlapping some of our measurements.
  We also consider Population II models: low-metallicity core-collapse SNe from M.
  Limongi & A. Chieffi (2018; orange contours, Population II SNe (L18)) occupy −0.25
  ≲ [C/O] ≲ 0.5 and −0.4 ≲ [Si/O] ≲ 0.4, overlapping parts of the Population III range,
  while the C. Kobayashi et al. (2006) yields (pink and orange circles for hypernovae
  and SNe, respectively) tend toward lower [Si/O] and [C/O].\r\n\r\nAgainst these
  predictions, the contrast between the two absorber populations is clear. All nongalaxy
  O i systems (green crosses) fall at the lower left of the diagram, consistent with
  enrichment from both Population II and/or Population III SNe models. This regime
  also overlaps with ultra-metal-poor damped Lyman-α absorbers (DLAs) at z ∼ 3 (−0.5
  ≲ [Si/O] ≲ 0, −0.5 ≲ [C/O] ≲ 0; R. Cooke et al. 2011; R. J. Cooke et al. 2017).
  By contrast, three of the five galaxy-associated absorbers lie well outside both
  the locus of Population II predictions and the locus of ultra-metal-poor DLA relative
  abundances. These systems are best explained if Population III enrichment played
  a major role, suggesting that they may represent a distinct population from ultra-metal-poor
  DLA host galaxies (see also A. Sodini et al. 2024).\r\n\r\nSimilarly, A. Sodini
  et al. (2024) found that the [C/O] and [Si/O] abundance ratios for high-redshift
  O i absorber systems are consistent with significant enrichment from Population
  III, with the majority explained by ≥ 30% contributions. They also find a large
  spread in the implied Population III contribution; several systems require ≥ 60%
  contributions, while others fall significantly below the average. This is a strong
  indication of heterogeneous chemical enrichment by Population III stars during the
  epoch of reionization.\r\n\r\nThe absorber toward J159 at z = 5.91 shows [C/O] =
  0.20, [Si/O] = 0.55 (labeled c), and no evidence of high-ionization absorption.
  These abundance ratios are best explained by contributions from Population III SNe
  or hypernovae. The absorber toward J1030 at z = 6.07 ([C/O] = −0.38, [Si/O] = 0.65,
  labeled e) also shows no high-ionization absorption. The relative abundances in
  these two predominantly neutral systems are therefore quite robust. Interestingly,
  the J1030 system is not reproduced by any single Population II or Population III
  model, suggesting that it may have experienced multiple enrichment episodes, producing
  unusually high [Si/O] coupled with low [C/O].\r\n\r\nTwo cases require special mention.
  The absorber toward J0100 at z = 5.94 shows [C/O] ≥ 0.42 and [Si/O] ≥ 0.67 (labeled
  a), with strong C iv and Si iv absorption. Since these are lower limits, ionization
  corrections (for carbon and silicon) would push this system further upward, strengthening
  the case for Population III contributions. This observation is best explained by
  contributions from Population III hypernovae models. The J1148 absorber at z = 6.01
  shows [C/O] ≥ 0.02 and [Si/O] ≥ 0.20 (labeled b), again with high-ionization lines;
  correcting for ionization would shift it diagonally upward in the diagram. Taken
  together, four of the five galaxy-associated absorbers show relative abundances
  that cannot be explained by Population II models alone, pointing instead to significant
  enrichment from Population III SNe or hypernovae.\r\n\r\nThus, most galaxy-associated
  O i systems carry signatures of Population III enrichment. These results suggest
  that O i systems tracing galaxy overdensities at z ∼ 6 carry chemical signatures
  of Population III enrichment, likely from multiple SNe events rather than a single
  explosion. The elevated [Si/O] and [C/O] ratios in these environments imply that
  [O iii]—emitting galaxies at this epoch may retain significant Population III contributions,
  and that metal-line absorbers around such overdensities provide a powerful probe
  of the first generations of stars.\r\n\r\n4.4. Comparison to the z ≈ 0 Universe\r\nAt
  z ∼ 6, we cannot directly detect the local environments where O i absorption systems
  arise. However, at z ∼ 0, there are instances where the environments giving rise
  to O i absorption are well understood. Here, we discuss several such instances and
  compare them with z ∼ 6 observations. Such comparisons can provide useful insights
  regarding the nature of local environments within which O i systems exist at high
  z. We focus on O i absorption associated with local blue compact dwarf (BCD) galaxies
  and the Magellanic Stream (MS), owing to their low metallicities and well-characterized
  local environments.\r\n\r\nThere is evidence that O i is found preferentially in
  the H ii regions of local BCDs, with their H i regions being pristine or showing
  very low levels of enrichment (D. Kunth et al. 1994; M. Pettini & K. Lipman 1995;
  T. X. Thuan & Y. I. Izotov 1997). In particular, T. X. Thuan & Y. I. Izotov (1997)
  report that, to varying degrees, low-ionization metal lines (e.g., O i and Si ii)
  reside in the ionized hydrogen regions of BCDs rather than the neutral hydrogen
  regions. They report . Compared to the z ∼ 6 measurements in panel (b) of Figure
  7, the O i column density of the BCD is comparable, but the Si ii-to-O i ratio is
  inconsistent with the z ∼ 6 values. On the other hand, V. Lebouteiller et al. (2004)
  find that the H ii region of the BCD I Zw 36 has significantly higher metallicity
  than its H i region. However, inferred from velocity offsets, O i in that system
  is associated with the H i region. The reported O i column density of that BCD ()
  is approximately 2 orders of magnitude higher than the z ∼ 6 sample. Given the available
  evidence, we conclude that the observed z ∼ 6 O i absorption systems are not similar
  to local BCD systems and are unlikely to originate in H ii regions.\r\n\r\nThe MS
  is a filamentary trail of gas in the Local Group. Multiphase absorption-line observations
  from A. J. Fox et al. (2013) and P. Richter et al. (2013) support the argument that
  the MS was tidally stripped from the Magellanic Clouds approximately 2 Gyr ago.
  Inferences from the abundance ratios of alpha elements in the MS are best explained
  by contributions from massive stars via Type II SNe when the MS was still part of
  the Magellanic Clouds, although the presence of significant dust depletion makes
  further inferences into enrichment history difficult. An additional study of the
  MS (N. Kumari et al. 2015) reports abundance ratios in a compact high-velocity cloud
  (CHVC) that is believed to be associated with the MS. They find [Si/O] = −0.04 ±
  0.25 and [C/O] = −0.09 ± 0.23. When comparing these with the z ∼ 6 observations
  presented in panel (c) of Figure 7, we see that the CHVC abundance ratios occupy
  a different region of parameter space than the z ≈ 6 O i absorbers within identified
  galactic overdensities showing Population III enrichment signatures (points a, c,
  e). This discrepancy provides evidence that these z ∼ 6 O i absorbers with Population
  III enrichment signatures are unlikely to arise in environments similar to the MS.
  However, the ionic ratios of O i absorption systems not associated with galaxy overdensities
  (green crosses) are consistent with this measurement. With the caveat that MS measurements
  do contain dust depletion effects, it is plausible that such O i systems may trace
  IGM structures with densities comparable to those of the MS at high z.\r\n\r\n5.
  Conclusion\r\nWe have conducted a survey of neutral O i absorption systems associated
  with galaxies during the Epoch of Reionization in the EIGER survey, using six high-redshift
  quasars as background sight lines. Our study focuses on the distribution of neutral
  oxygen around -emitting galaxies within 300 kpc and their connection to galaxy overdensities.
  The main results are as follows:\r\n\r\n1.  \r\nFive O i absorbers are detected
  among 15 galaxy overdensities, spanning z = 5.91–6.16 with a mean redshift 〈z〉 =
  6.001.\r\n2.  \r\nThe O i covering fraction within 300 kpc of the closest galaxy
  is , with for R ≤ 50 kpc and for 50 ≤ R ≤ 300 kpc, where the covering fraction is
  calculated using the galaxy in an overdensity with the lowest impact parameter.\r\n3.
  \ \r\nWe find  ≳ 2 × 106 M⊙ of oxygen within 300 kpc, a mass comparable to the ISM
  oxygen content of z ∼ 6 galaxies—assuming minimal ionization correction (see Section
  4.1 for justification)—suggesting that the circumgalactic environment already holds
  metal reservoirs rivaling those inside galaxies.\r\n4.  \r\nO i absorbers are detected
  as far as ∼8 R/Rvir from galaxies, in sharp contrast to low-ionization tracers such
  as Mg ii, which are typically confined within ≲R/Rvir.\r\n5.  \r\nThe incidence
  of galaxy-associated O i absorbers is \r\n \r\n. Comparison with blind quasar absorption-line
  surveys indicates that these systems represent only ∼35% of all O i absorbers at
  z ∼ 6, implying that the majority likely arise in lower-mass galaxies below current
  detection limits or in dense neutral IGM pockets that survived reionization.\r\n6.
  \ \r\nRelative abundance and ionization ratios ([Si/O], [C/O]) show that galaxy-associated
  O i systems are chemically enriched, with signatures in several systems consistent
  with contributions from Population III stars. In particular, we identify four galaxy
  overdensities whose outskirts exhibit absorption-line abundance ratios consistent
  with contributions from Population III nucleosynthesis.\r\n\r\nOverall, these results
  indicate that neutral O i at z ∼ 6 primarily traces extended overdensity environments
  rather than the CGM of individual halos. Moreover, the chemical abundance patterns
  of galaxy-associated O i systems suggest contributions from Population III stars,
  likely arising from multiple SNe events rather than a single explosion. The elevated
  [Si/O] and [C/O] ratios imply that [O iii]-emitting galaxies at this epoch may retain
  significant Population III enrichment. Consequently, metal-line absorbers around
  such overdensities offer a powerful probe of the first generations of stars, providing
  insight into early chemical enrichment and the role of primordial stellar populations
  in shaping galaxy evolution during the Epoch of Reionization.\r\n\r\nAcknowledgments\r\nThis
  work is based on observations made with the NASA/ESA/CSA James Webb Space Telescope.
  The data were obtained from the Mikulski Archive for Space Telescopes at the Space
  Telescope Science Institute, which is operated by the Association of Universities
  for Research in Astronomy, Inc., under NASA contract NAS 5-03127 for JWST. These
  observations are associated with program #1243. This paper includes data gathered
  with the 6.5 m Magellan Telescopes located at Las Campanas Observatory, Chile. This
  work was supported by a NASA Keck PI Data Award, administered by the NASA Exoplanet
  Science Institute. Data presented herein were obtained at the W. M. Keck Observatory
  from telescope time allocated to the National Aeronautics and Space Administration
  (NASA) through the agency’s scientific partnership with the California Institute
  of Technology and the University of California. The Observatory was made possible
  by the generous financial support of the W. M. Keck Foundation. 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/y94q-h212. This work was partially supported by the
  National Science Foundation under grant No. AST-2108931. Jorryt Matthee and Ivan
  Kramarenko acknowledge funding from the European Union (ERC, AGENTS, 101076224).\r\n\r\nFacilities:
  JWST - James Webb Space Telescope (NIRCam), Magellan: Baade - (FIRE), VLT: Kueyen
  - (X-shooter), and Keck: I - (HIRES, MOSFIRE).\r\n\r\nSoftware: astropy (Astropy
  Collaboration et al. 2013, 2018, 2022), rbcodes (R. Bordoloi et al. 2025), rbvfit
  (R. Bordoloi & J. Higginson 2025)."
article_number: '49'
article_processing_charge: Yes
article_type: original
arxiv: 1
author:
- first_name: Jack
  full_name: Higginson, Jack
  last_name: Higginson
- first_name: Rongmon
  full_name: Bordoloi, Rongmon
  last_name: Bordoloi
- first_name: Robert A.
  full_name: Simcoe, Robert A.
  last_name: Simcoe
- 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: Daichi
  full_name: Kashino, Daichi
  last_name: Kashino
- first_name: Ruari
  full_name: Mackenzie, Ruari
  last_name: Mackenzie
- first_name: Ivan
  full_name: Kramarenko, Ivan
  id: 9a9394cb-3200-11ee-973b-f5ba2a8b16e4
  last_name: Kramarenko
  orcid: 0000-0001-5346-6048
- first_name: Simon J.
  full_name: Lilly, Simon J.
  last_name: Lilly
- first_name: Anna-Christina
  full_name: Eilers, Anna-Christina
  last_name: Eilers
- first_name: Rohan P.
  full_name: Naidu, Rohan P.
  last_name: Naidu
- first_name: Minghao
  full_name: Yue, Minghao
  last_name: Yue
citation:
  ama: Higginson J, Bordoloi R, Simcoe RA, et al. EIGER. VIII. First stars signatures
    in the connection between O I absorption and galaxies in the epoch of reionization.
    <i>The Astrophysical Journal</i>. 2026;999(1). doi:<a href="https://doi.org/10.3847/1538-4357/ae3e81">10.3847/1538-4357/ae3e81</a>
  apa: Higginson, J., Bordoloi, R., Simcoe, R. A., Matthee, J. J., Kashino, D., Mackenzie,
    R., … Yue, M. (2026). EIGER. VIII. First stars signatures in the connection between
    O I absorption and galaxies in the epoch of reionization. <i>The Astrophysical
    Journal</i>. IOP Publishing. <a href="https://doi.org/10.3847/1538-4357/ae3e81">https://doi.org/10.3847/1538-4357/ae3e81</a>
  chicago: Higginson, Jack, Rongmon Bordoloi, Robert A. Simcoe, Jorryt J Matthee,
    Daichi Kashino, Ruari Mackenzie, Ivan Kramarenko, et al. “EIGER. VIII. First Stars
    Signatures in the Connection between O I Absorption and Galaxies in the Epoch
    of Reionization.” <i>The Astrophysical Journal</i>. IOP Publishing, 2026. <a href="https://doi.org/10.3847/1538-4357/ae3e81">https://doi.org/10.3847/1538-4357/ae3e81</a>.
  ieee: J. Higginson <i>et al.</i>, “EIGER. VIII. First stars signatures in the connection
    between O I absorption and galaxies in the epoch of reionization,” <i>The Astrophysical
    Journal</i>, vol. 999, no. 1. IOP Publishing, 2026.
  ista: Higginson J, Bordoloi R, Simcoe RA, Matthee JJ, Kashino D, Mackenzie R, Kramarenko
    I, Lilly SJ, Eilers A-C, Naidu RP, Yue M. 2026. EIGER. VIII. First stars signatures
    in the connection between O I absorption and galaxies in the epoch of reionization.
    The Astrophysical Journal. 999(1), 49.
  mla: Higginson, Jack, et al. “EIGER. VIII. First Stars Signatures in the Connection
    between O I Absorption and Galaxies in the Epoch of Reionization.” <i>The Astrophysical
    Journal</i>, vol. 999, no. 1, 49, IOP Publishing, 2026, doi:<a href="https://doi.org/10.3847/1538-4357/ae3e81">10.3847/1538-4357/ae3e81</a>.
  short: J. Higginson, R. Bordoloi, R.A. Simcoe, J.J. Matthee, D. Kashino, R. Mackenzie,
    I. Kramarenko, S.J. Lilly, A.-C. Eilers, R.P. Naidu, M. Yue, The Astrophysical
    Journal 999 (2026).
date_created: 2026-10-12T12:15:27Z
date_published: 2026-02-24T00:00:00Z
date_updated: 2026-10-14T07:58:57Z
day: '24'
ddc:
- '520'
department:
- _id: JoMa
- _id: GradSch
doi: 10.3847/1538-4357/ae3e81
external_id:
  arxiv:
  - '2510.05220'
file:
- access_level: open_access
  checksum: 1b8caf640c32d0d27a078bfb27ffcf8a
  content_type: application/pdf
  creator: dernst
  date_created: 2026-10-14T07:50:51Z
  date_updated: 2026-10-14T07:50:51Z
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  file_size: 2808503
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  success: 1
file_date_updated: 2026-10-14T07:50:51Z
fulldoi: https://doi.org/10.3847/1538-4357/ae3e81
has_accepted_license: '1'
intvolume: '       999'
issue: '1'
language:
- iso: eng
month: '02'
oa: 1
oa_version: Published Version
project:
- _id: bd9b2118-d553-11ed-ba76-db24564edfea
  grant_number: '101076224'
  name: Young galaxies as tracers and agents of cosmic reionization
publication: The Astrophysical Journal
publication_identifier:
  eissn:
  - 1538-4357
  issn:
  - 0004-637X
publication_status: published
publisher: IOP Publishing
quality_controlled: '1'
scopus_import: '1'
status: public
title: EIGER. VIII. First stars signatures in the connection between O I absorption
  and galaxies in the epoch of reionization
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: 999
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '23117'
abstract:
- lang: eng
  text: 'We present a comprehensive analysis of the relationship between galaxies
    and the intergalactic medium (IGM) during the late stages of cosmic reionization,
    based on the complete JWST EIGER dataset. Using deep NIRCam 3.5 μm slitless spectroscopy,
    we construct a sample of 948 [O iii]λ5008-emitting galaxies with −21.4 ≲ MUV ≲
    −17.2 spanning 5.33 < z < 6.97 along six quasar sight lines. We correlate these
    galaxies with Lyα and Lyβ transmission measured from high-resolution quasar spectra
    across multiple redshift intervals. We find clear redshift evolution in the correlation
    between galaxy density and transmission: it is suppressed in overdense regions
    at z < 5.50, while enhanced at 5.70 < z < 6.15. The intermediate range exhibits
    a transitional behavior. Cross-correlation measurements further reveal excess
    absorption within ∼8 cMpc of galaxies at low redshifts, and enhanced transmission
    at intermediate scales (∼5–20 cMpc) at z > 5.70. Statistical tests using mock
    catalogs with realistic galaxy clustering but no correlation with the transmission
    field confirm that the observed correlations are unlikely to arise by chance.
    The evolving signals can be explained by stronger absorption in overdense regions,
    combined with the competing influences of local radiation fields and the rising
    background radiation. While local radiation dominates ionization of the surrounding
    IGM at earlier times, the background becomes increasingly important, eventually
    surpassing the impact of nearby galaxies. These results support an inside-out
    progression of reionization, with ionized regions originating around clustered,
    star-forming galaxies and gradually extending into underdense regions.'
acknowledgement: "We thank Enrico Garaldi, Rahul Kannan, Aaron Smith, and the THESAN
  team for providing us with their simulation data, and Norbert Pirzkal for helpful
  advice on our NIRCam observing program.\r\n\r\nThis work is based on observations
  made with the NASA/ESA/CSA James Webb Space Telescope. The data were obtained from
  the Mikulski Archive for Space Telescopes at the Space Telescope Science Institute,
  which is operated by the Association of Universities for Research in Astronomy,
  Inc., under NASA contract NAS 5-03127 for JWST. These observations were taken under
  GTO program No. 1243. The specific observations analyzed can be accessed via doi:10.17909/6grb-j154.\r\n\r\nThe
  participation of S.J.L. as an Interdisciplinary Scientist in the JWST Flight Science
  Working Group 2002-2022 has been supported by the European Space Agency. His earlier
  involvement in the development of the JWST 1996–2001 was supported by the Canadian
  Space Agency.\r\n\r\nThis work is partially based on observations collected at the
  European Organisation for Astronomical Research in the Southern Hemisphere under
  ESO programmes 084.A-0360(A), 084.A-0390(A), 086.A-0162(A), 086.A-0574(A), 087.A-0607(A),
  089.A-0814(A), 093.A-0707(A), 098.B-0537(A), and 286.A-5025(A). Some of the data
  presented herein were obtained at Keck Observatory, which is a private 501(c)3 nonprofit
  organization operated as a scientific partnership among the California Institute
  of Technology, the University of California, and the National Aeronautics and Space
  Administration. The Observatory was made possible by the generous financial support
  of the W. M. Keck Foundation. This paper includes data gathered with the 6.5 m Magellan
  Telescopes located at Las Campanas Observatory, Chile.\r\n\r\nThis work has been
  supported by JSPS KAKENHI grant No. JP21K13956 (D.K.). J.M. is supported by the
  European Union (ERC, AGENTS, 101076224).\r\n\r\nFacilities: JWST - James Webb Space
  Telescope (NIRCam), VLT:Kueyen - Very Large Telescope (Kueyen) (X-Shooter), Magellan:Baade
  - Magellan I Walter Baade Telescope (FIRE), Keck:I - KECK I Telescope (MOSFIRE),
  Keck:II - KECK II Telescope (ESI).\r\n\r\nSoftware: Python, numpy (C. R. Harris
  et al. 2020), scipy (P. Virtanen et al. 2020), Astropy (Astropy Collaboration et
  al. 2013), Matplotlib (J. D. Hunter 2007), PypeIt (J. X. Prochaska et al. 2019)."
article_number: '280'
article_processing_charge: Yes
article_type: original
arxiv: 1
author:
- first_name: Daichi
  full_name: Kashino, Daichi
  last_name: Kashino
- first_name: Simon J.
  full_name: Lilly, Simon J.
  last_name: Lilly
- 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: Ruari
  full_name: Mackenzie, Ruari
  last_name: Mackenzie
- first_name: Anna-Christina
  full_name: Eilers, Anna-Christina
  last_name: Eilers
- first_name: Rongmon
  full_name: Bordoloi, Rongmon
  last_name: Bordoloi
- first_name: Robert A.
  full_name: Simcoe, Robert A.
  last_name: Simcoe
- first_name: Rohan P.
  full_name: Naidu, Rohan P.
  last_name: Naidu
- first_name: Minghao
  full_name: Yue, Minghao
  last_name: Yue
- first_name: Bin
  full_name: Liu, Bin
  last_name: Liu
citation:
  ama: Kashino D, Lilly SJ, Matthee JJ, et al. EIGER. VII. The evolving relationship
    between galaxies and the intergalactic medium in the final stages of reionization.
    <i>The Astrophysical Journal</i>. 2026;997(2). doi:<a href="https://doi.org/10.3847/1538-4357/ae2799">10.3847/1538-4357/ae2799</a>
  apa: Kashino, D., Lilly, S. J., Matthee, J. J., Mackenzie, R., Eilers, A.-C., Bordoloi,
    R., … Liu, B. (2026). EIGER. VII. The evolving relationship between galaxies and
    the intergalactic medium in the final stages of reionization. <i>The Astrophysical
    Journal</i>. IOP Publishing. <a href="https://doi.org/10.3847/1538-4357/ae2799">https://doi.org/10.3847/1538-4357/ae2799</a>
  chicago: Kashino, Daichi, Simon J. Lilly, Jorryt J Matthee, Ruari Mackenzie, Anna-Christina
    Eilers, Rongmon Bordoloi, Robert A. Simcoe, Rohan P. Naidu, Minghao Yue, and Bin
    Liu. “EIGER. VII. The Evolving Relationship between Galaxies and the Intergalactic
    Medium in the Final Stages of Reionization.” <i>The Astrophysical Journal</i>.
    IOP Publishing, 2026. <a href="https://doi.org/10.3847/1538-4357/ae2799">https://doi.org/10.3847/1538-4357/ae2799</a>.
  ieee: D. Kashino <i>et al.</i>, “EIGER. VII. The evolving relationship between galaxies
    and the intergalactic medium in the final stages of reionization,” <i>The Astrophysical
    Journal</i>, vol. 997, no. 2. IOP Publishing, 2026.
  ista: Kashino D, Lilly SJ, Matthee JJ, Mackenzie R, Eilers A-C, Bordoloi R, Simcoe
    RA, Naidu RP, Yue M, Liu B. 2026. EIGER. VII. The evolving relationship between
    galaxies and the intergalactic medium in the final stages of reionization. The
    Astrophysical Journal. 997(2), 280.
  mla: Kashino, Daichi, et al. “EIGER. VII. The Evolving Relationship between Galaxies
    and the Intergalactic Medium in the Final Stages of Reionization.” <i>The Astrophysical
    Journal</i>, vol. 997, no. 2, 280, IOP Publishing, 2026, doi:<a href="https://doi.org/10.3847/1538-4357/ae2799">10.3847/1538-4357/ae2799</a>.
  short: D. Kashino, S.J. Lilly, J.J. Matthee, R. Mackenzie, A.-C. Eilers, R. Bordoloi,
    R.A. Simcoe, R.P. Naidu, M. Yue, B. Liu, The Astrophysical Journal 997 (2026).
das_tickbox: '0'
date_created: 2026-10-12T12:17:25Z
date_published: 2026-01-28T00:00:00Z
date_updated: 2026-10-14T08:12:05Z
day: '28'
ddc:
- '520'
department:
- _id: JoMa
doi: 10.3847/1538-4357/ae2799
external_id:
  arxiv:
  - '2506.03121'
file:
- access_level: open_access
  checksum: c33405da323cac352c0d751f0fe6f021
  content_type: application/pdf
  creator: dernst
  date_created: 2026-10-14T08:09:31Z
  date_updated: 2026-10-14T08:09:31Z
  file_id: '23138'
  file_name: 2026_AstrophysicalJour_Kashino.pdf
  file_size: 11393255
  relation: main_file
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file_date_updated: 2026-10-14T08:09:31Z
fulldoi: https://doi.org/10.3847/1538-4357/ae2799
has_accepted_license: '1'
intvolume: '       997'
issue: '2'
language:
- iso: eng
month: '01'
oa: 1
oa_version: Published Version
project:
- _id: bd9b2118-d553-11ed-ba76-db24564edfea
  grant_number: '101076224'
  name: Young galaxies as tracers and agents of cosmic reionization
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: yes
title: EIGER. VII. The evolving relationship between galaxies and the intergalactic
  medium in the final stages of reionization
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: 997
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '23111'
abstract:
- lang: eng
  text: In single-molecule electronics, 4,4′-bipyridine is a well-characterized molecule
    that serves both as a fundamental testbed for developing experimental methodologies
    and showcases the complex behaviors expected from molecular electronic components.
    In break junction experiments, it is generally understood to exhibit a high- and
    a low-conductance state that are attributed to a tilted and stretched single-molecule
    configuration. Despite this established view, we suggest a supramolecular origin
    for these conductance states that has not previously been considered. Our findings
    indicate that the high- and low-conductance states may arise from the presence
    of two molecules and one molecule, respectively, challenging the conventional
    interpretation. Using a state-of-the-art machine learning force field called the
    neuroevolution potential, we find that the conventional interpretation of a tilted
    and stretched configuration is inconsistent with our simulations. Instead, our
    results suggest that the presence of two molecules promotes junction geometries
    and gold rearrangements that stabilize a high-conductance state whose transmission
    exceeds twice that of the low-conductance state. Furthermore, we compare this
    interpretation to the existing literature of diverse experimental data on 4,4′-bipyridine
    in break junctions and find that it is consistent with the broader body of experimental
    evidence. Our results highlight the structural complexity of molecular behavior
    within break junctions, suggesting even more complex dynamics than originally
    anticipated. In this light, a broader examination of the dynamics of molecules
    in single-molecule break junctions with machine learning-assisted molecular dynamics
    is warranted.
acknowledgement: The authors thank Latha Venkataraman for fruitful discussions about
  the main results of this paper. This project has received funding from the European
  Research Council (ERC) under the European Union’s Horizon 2020 research and innovation
  programme (grant agreement No. 865870). Junfeng Lin thanks the Institute of Science
  and Technology Austria for support.
article_processing_charge: Yes
article_type: original
author:
- first_name: William
  full_name: Bro-Jørgensen, William
  last_name: Bro-Jørgensen
- first_name: Junfeng
  full_name: Lin, Junfeng
  id: a25c6e57-a657-11ef-8665-c4906b069ffc
  last_name: Lin
- first_name: Joseph M.
  full_name: Hamill, Joseph M.
  last_name: Hamill
- first_name: Gemma C.
  full_name: Solomon, Gemma C.
  last_name: Solomon
chemrxivid: 1
citation:
  ama: 'Bro-Jørgensen W, Lin J, Hamill JM, Solomon GC. Machine learning-enhanced molecular
    dynamics of 4,4′-bipyridinein a break junction: A supramolecular origin of the
    high conductance. <i>ACS Nanoscience Au</i>. 2026;6(4):662-673. doi:<a href="https://doi.org/10.1021/acsnanoscienceau.6c00052">10.1021/acsnanoscienceau.6c00052</a>'
  apa: 'Bro-Jørgensen, W., Lin, J., Hamill, J. M., &#38; Solomon, G. C. (2026). Machine
    learning-enhanced molecular dynamics of 4,4′-bipyridinein a break junction: A
    supramolecular origin of the high conductance. <i>ACS Nanoscience Au</i>. American
    Chemical Society. <a href="https://doi.org/10.1021/acsnanoscienceau.6c00052">https://doi.org/10.1021/acsnanoscienceau.6c00052</a>'
  chicago: 'Bro-Jørgensen, William, Junfeng Lin, Joseph M. Hamill, and Gemma C. Solomon.
    “Machine Learning-Enhanced Molecular Dynamics of 4,4′-Bipyridinein a Break Junction:
    A Supramolecular Origin of the High Conductance.” <i>ACS Nanoscience Au</i>. American
    Chemical Society, 2026. <a href="https://doi.org/10.1021/acsnanoscienceau.6c00052">https://doi.org/10.1021/acsnanoscienceau.6c00052</a>.'
  ieee: 'W. Bro-Jørgensen, J. Lin, J. M. Hamill, and G. C. Solomon, “Machine learning-enhanced
    molecular dynamics of 4,4′-bipyridinein a break junction: A supramolecular origin
    of the high conductance,” <i>ACS Nanoscience Au</i>, vol. 6, no. 4. American Chemical
    Society, pp. 662–673, 2026.'
  ista: 'Bro-Jørgensen W, Lin J, Hamill JM, Solomon GC. 2026. Machine learning-enhanced
    molecular dynamics of 4,4′-bipyridinein a break junction: A supramolecular origin
    of the high conductance. ACS Nanoscience Au. 6(4), 662–673.'
  mla: 'Bro-Jørgensen, William, et al. “Machine Learning-Enhanced Molecular Dynamics
    of 4,4′-Bipyridinein a Break Junction: A Supramolecular Origin of the High Conductance.”
    <i>ACS Nanoscience Au</i>, vol. 6, no. 4, American Chemical Society, 2026, pp.
    662–73, doi:<a href="https://doi.org/10.1021/acsnanoscienceau.6c00052">10.1021/acsnanoscienceau.6c00052</a>.'
  short: W. Bro-Jørgensen, J. Lin, J.M. Hamill, G.C. Solomon, ACS Nanoscience Au 6
    (2026) 662–673.
das_tickbox: '1'
dataavailabilitystatement: 'Input and output files for the MD trajectories are available
  in our ioChem-BD repository (85) and can be accessed here: 10.19061/iochem-bd-9-14.
  Raw data for all MD trajectories are available here: 10.17894/ucph.78aa9ec7-d132-447f-aaf0-8e6e5d59d8ea'
date_created: 2026-10-12T12:01:45Z
date_published: 2026-08-19T00:00:00Z
date_updated: 2026-10-14T07:09:01Z
day: '19'
ddc:
- '540'
department:
- _id: LaVe
doi: 10.1021/acsnanoscienceau.6c00052
external_id:
  chemrxivid:
  - 10.26434/chemrxiv-2025-wt6rd/v2
  pmid:
  - '42630769'
file:
- access_level: open_access
  checksum: 87cc93f52ba508a7d19d7c03e9ef55cb
  content_type: application/pdf
  creator: dernst
  date_created: 2026-10-14T07:07:43Z
  date_updated: 2026-10-14T07:07:43Z
  file_id: '23135'
  file_name: 2026_ACSNanoscienceAu_BroJorgensen.pdf
  file_size: 6463446
  relation: main_file
  success: 1
file_date_updated: 2026-10-14T07:07:43Z
fulldoi: https://doi.org/10.1021/acsnanoscienceau.6c00052
has_accepted_license: '1'
intvolume: '         6'
issue: '4'
language:
- iso: eng
month: '08'
oa: 1
oa_version: Published Version
page: 662-673
pmid: 1
publication: ACS Nanoscience Au
publication_identifier:
  issn:
  - 2694-2496
publication_status: published
publisher: American Chemical Society
quality_controlled: '1'
researchdata_availability: yes
scopus_import: '1'
status: public
supplementarymaterial: yes
title: 'Machine learning-enhanced molecular dynamics of 4,4′-bipyridinein a break
  junction: A supramolecular origin of the high conductance'
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: 6
year: '2026'
...
---
DOAJ_listed: '1'
OA_place: publisher
OA_type: gold
PlanS_conform: '1'
_id: '23116'
abstract:
- lang: eng
  text: The Legacy Survey of Space and Time (LSST) is expected to observe up to ∼100
    million quasars in the next decade. In this work, we show that it is possible
    to use such data to measure the characteristic frequency evolution of a “chirp”
    induced by gravitational waves, which can serve as robust evidence for the presence
    of a compact supermassive black hole binary. Following the LSST specifications,
    we generate mock lightcurves consisting of (i) a post-Newtonian chirp produced
    by orbital motion through, e.g., relativistic Doppler boosting, (ii) a damped
    random walk representing intrinsic quasar variability, and (iii) Gaussian photometric
    errors, while assuming nonuniform observations with extended gaps over a period
    of 10 yr. Through a fully Bayesian analysis, we show that we can simultaneously
    measure the chirp and noise parameters with little degeneracy between the two.
    For chirp signals with an amplitude of A = 0.5 mag and a range of times to merger
    (tm = 15–104 yr), we can typically measure a nonzero amplitude and positive frequency
    derivative with over 5σ credibility. For binaries with tm = 50 yr, we achieve
    3σ (5σ) confidence that the signal is chirping for A ≳ 0.1 (A  >  0.2). The median
    runtime of our analysis is 5.6 minutes, with a minimum as low as 35 s, making
    it scalable to a large number of lightcurves. This implies that LSST could, on
    its own, establish the presence of a compact supermassive black hole binary, and
    thus discover gravitational wave sources detectable by LISA and by Pulsar Timing
    Arrays.
acknowledgement: "C.X. thanks the Department of Astronomy of Columbia University,
  where the majority of this work was performed. Z.H. thanks the Center for Computational
  Astrophysics (CCA) at the Flatiron Institute for their hospitality during a sabbatical
  stay, where this work was initiated. The Flatiron Institute is a division of the
  Simons Foundation. This work was supported in part by NASA’s LISA Preparatory Science
  Program (LPS) through grant 80NSSC24K0440 and by NASA Astrophysics Theory Program
  (ATP) grant 80NSSC22K0822. The authors thank the anonymous referee for helpful feedback,
  which improved this manuscript. We also thank Prof. Brian D. Metzger, Prof. David
  Schiminovich, and Prof. Kishalay De for valuable discussions.\r\n\r\nSoftware: numpyro
  (E. Bingham et al. 2019; D. Phan et al. 2019); celerite2 (D. Foreman-Mackey et al.
  2017; D. Foreman-Mackey 2018); Python (G. Van Rossum & F. L. Drake 2009); The Software
  Citation Station (T. Wagg & F. S. Broekgaarden 2024; T. Wagg et al. 2024)."
article_number: '149'
article_processing_charge: Yes
article_type: original
arxiv: 1
author:
- first_name: Chengcheng
  full_name: Xin, Chengcheng
  last_name: Xin
- first_name: Maximiliano
  full_name: Isi, Maximiliano
  last_name: Isi
- first_name: Will M.
  full_name: Farr, Will M.
  last_name: Farr
- first_name: Zoltán
  full_name: Haiman, Zoltán
  id: 7c006e8c-cc0d-11ee-8322-cb904ef76f36
  last_name: Haiman
  orcid: 0000-0003-3633-5403
citation:
  ama: Xin C, Isi M, Farr WM, Haiman Z. Identifying compact chirping SMBHBs in LSST
    using Bayesian analysis. <i>The Astrophysical Journal</i>. 2026;999(1). doi:<a
    href="https://doi.org/10.3847/1538-4357/ae40b3">10.3847/1538-4357/ae40b3</a>
  apa: Xin, C., Isi, M., Farr, W. M., &#38; Haiman, Z. (2026). Identifying compact
    chirping SMBHBs in LSST using Bayesian analysis. <i>The Astrophysical Journal</i>.
    IOP Publishing. <a href="https://doi.org/10.3847/1538-4357/ae40b3">https://doi.org/10.3847/1538-4357/ae40b3</a>
  chicago: Xin, Chengcheng, Maximiliano Isi, Will M. Farr, and Zoltán Haiman. “Identifying
    Compact Chirping SMBHBs in LSST Using Bayesian Analysis.” <i>The Astrophysical
    Journal</i>. IOP Publishing, 2026. <a href="https://doi.org/10.3847/1538-4357/ae40b3">https://doi.org/10.3847/1538-4357/ae40b3</a>.
  ieee: C. Xin, M. Isi, W. M. Farr, and Z. Haiman, “Identifying compact chirping SMBHBs
    in LSST using Bayesian analysis,” <i>The Astrophysical Journal</i>, vol. 999,
    no. 1. IOP Publishing, 2026.
  ista: Xin C, Isi M, Farr WM, Haiman Z. 2026. Identifying compact chirping SMBHBs
    in LSST using Bayesian analysis. The Astrophysical Journal. 999(1), 149.
  mla: Xin, Chengcheng, et al. “Identifying Compact Chirping SMBHBs in LSST Using
    Bayesian Analysis.” <i>The Astrophysical Journal</i>, vol. 999, no. 1, 149, IOP
    Publishing, 2026, doi:<a href="https://doi.org/10.3847/1538-4357/ae40b3">10.3847/1538-4357/ae40b3</a>.
  short: C. Xin, M. Isi, W.M. Farr, Z. Haiman, The Astrophysical Journal 999 (2026).
das_tickbox: '0'
date_created: 2026-10-12T12:16:19Z
date_published: 2026-02-27T00:00:00Z
date_updated: 2026-10-14T08:05:50Z
day: '27'
ddc:
- '520'
department:
- _id: ZoHa
doi: 10.3847/1538-4357/ae40b3
external_id:
  arxiv:
  - '2506.10846'
file:
- access_level: open_access
  checksum: 250ede2883cf2e3ec9ac8c36b1857d40
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  creator: dernst
  date_created: 2026-10-14T08:02:55Z
  date_updated: 2026-10-14T08:02:55Z
  file_id: '23137'
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  file_size: 4415354
  relation: main_file
  success: 1
file_date_updated: 2026-10-14T08:02:55Z
fulldoi: https://doi.org/10.3847/1538-4357/ae40b3
has_accepted_license: '1'
intvolume: '       999'
issue: '1'
language:
- iso: eng
month: '02'
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: yes
title: Identifying compact chirping SMBHBs in LSST using Bayesian 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: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 999
year: '2026'
...
---
OA_type: closed access
_id: '23096'
abstract:
- lang: eng
  text: The first generation of stars, known as population III (Pop III), formed from
    primordial gas consisting solely of hydrogen and helium and is believed to have
    emerged only a few hundred million years after the Big Bang. Detecting the chemical
    enrichment of metal-poor circumgalactic gas offers a promising way to trace the
    enrichment signature of Pop III stars. Along the sight line to the quasar SDSS
    J0100+2802, a metal absorber at z = 5.945, showing over-abundant carbon and silicon
    compared with solar, has been reported to be consistent with the enrichment pattern
    of Pop III stars. Here, using data recorded by the James Webb Space Telescope,
    we report the discovery of an unusually metal-poor galaxy overdensity of 17 members
    (mean metallicity ~3% of solar) near this metal absorber, which is ~0.4 dex more
    metal-poor than coeval galaxies in similarly overdense environments. This less
    chemically evolved system may have provided favourable conditions for preserving
    the absorption signatures of Pop III enrichment. We infer a minimum dark matter
    halo mass of log(Mh,min/M⊙) = 10.68+0.93 −1.72, supporting late-time Pop III formation
    at the outskirts of atomic hydrogen cooling haloes. Our findings open a promising
    observational pathway to identifying the chemical imprints of the first stars
    and constrain the conditions for their formation.
acknowledgement: This work is based on observations made with the NASA/ESA/CSA JWST,
  associated with the programmes GO-1243 and GO-2078, and the Very Large Telescope,
  associated with ESO programmes X-shooter 0100.A-0625, 0102.A-0154, 1103.A-0817 and
  096.A-0095. We acknowledge the University of Copenhagen for giving this project
  access to the LUMI supercomputer owned by the EuroHPC Joint Undertaking and hosted
  by CSC (Finland) and the LUMI consortium through Denmark. Z.L. thanks Y. Ren for
  helpful discussions. We thank O. Zier, A. Smith, R. Kannan and E. Garaldi for helpful
  discussions about the THESAN-ZOOM simulation. Z.L. acknowledges the fellowship from
  the Cosmic Dawn Center, which is funded by the Danish National Research Foundation
  under grant no. 140. K.K. acknowledges support from the Villum Foundation (71574).
  L.C. is supported by DFF/Independent Research Fund Denmark (2032-00071). V.D. acknowledges
  financial support from the Bando Ricerca Fondamentale INAF 2022 Large Grant XQR-30.
  A.V. acknowledges funding from the Cosmic Frontier Center and the University of
  Texas at Austin’s College of Natural Sciences. S. Zou acknowledges support from
  the Chinese Academy of Sciences (E5295401).
article_processing_charge: No
article_type: original
author:
- first_name: Zihao
  full_name: Li, Zihao
  last_name: Li
- first_name: Koki
  full_name: Kakiichi, Koki
  last_name: Kakiichi
- first_name: Lise
  full_name: Christensen, Lise
  last_name: Christensen
- first_name: Zheng
  full_name: Cai, Zheng
  last_name: Cai
- first_name: Valentina
  full_name: D’Odorico, Valentina
  last_name: D’Odorico
- 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: Daichi
  full_name: Kashino, Daichi
  last_name: Kashino
- first_name: Rongmon
  full_name: Bordoloi, Rongmon
  last_name: Bordoloi
- first_name: Ruari
  full_name: Mackenzie, Ruari
  last_name: Mackenzie
- first_name: Trystyn A.M.
  full_name: Berg, Trystyn A.M.
  last_name: Berg
- first_name: Irene
  full_name: Vanni, Irene
  last_name: Vanni
- first_name: Stefania
  full_name: Salvadori, Stefania
  last_name: Salvadori
- first_name: Alessandra
  full_name: Venditti, Alessandra
  last_name: Venditti
- first_name: Shiwu
  full_name: Zhang, Shiwu
  last_name: Zhang
- first_name: Sarah E.I.
  full_name: Bosman, Sarah E.I.
  last_name: Bosman
- first_name: Eduardo
  full_name: Bañados, Eduardo
  last_name: Bañados
- first_name: Frederick B.
  full_name: Davies, Frederick B.
  last_name: Davies
- first_name: Xiaohui
  full_name: Fan, Xiaohui
  last_name: Fan
- first_name: Hyunsung D.
  full_name: Jun, Hyunsung D.
  last_name: Jun
- first_name: Xiangyu
  full_name: Jin, Xiangyu
  last_name: Jin
- first_name: Mingyu
  full_name: Li, Mingyu
  last_name: Li
- first_name: Sofía
  full_name: Rojas-Ruiz, Sofía
  last_name: Rojas-Ruiz
- first_name: Feige
  full_name: Wang, Feige
  last_name: Wang
- first_name: Jinyi
  full_name: Yang, Jinyi
  last_name: Yang
- first_name: Siwei
  full_name: Zou, Siwei
  last_name: Zou
- first_name: Huanian
  full_name: Zhang, Huanian
  last_name: Zhang
- first_name: Yongda
  full_name: Zhu, Yongda
  last_name: Zhu
citation:
  ama: Li Z, Kakiichi K, Christensen L, et al. First-star imprints in a metal-poor
    galaxy overdensity near the end of reionization. <i>Nature Astronomy</i>. 2026.
    doi:<a href="https://doi.org/10.1038/s41550-026-02993-5">10.1038/s41550-026-02993-5</a>
  apa: Li, Z., Kakiichi, K., Christensen, L., Cai, Z., D’Odorico, V., Matthee, J.
    J., … Zhu, Y. (2026). First-star imprints in a metal-poor galaxy overdensity near
    the end of reionization. <i>Nature Astronomy</i>. Springer Nature. <a href="https://doi.org/10.1038/s41550-026-02993-5">https://doi.org/10.1038/s41550-026-02993-5</a>
  chicago: Li, Zihao, Koki Kakiichi, Lise Christensen, Zheng Cai, Valentina D’Odorico,
    Jorryt J Matthee, Daichi Kashino, et al. “First-Star Imprints in a Metal-Poor
    Galaxy Overdensity near the End of Reionization.” <i>Nature Astronomy</i>. Springer
    Nature, 2026. <a href="https://doi.org/10.1038/s41550-026-02993-5">https://doi.org/10.1038/s41550-026-02993-5</a>.
  ieee: Z. Li <i>et al.</i>, “First-star imprints in a metal-poor galaxy overdensity
    near the end of reionization,” <i>Nature Astronomy</i>. Springer Nature, 2026.
  ista: Li Z, Kakiichi K, Christensen L, Cai Z, D’Odorico V, Matthee JJ, Kashino D,
    Bordoloi R, Mackenzie R, Berg TAM, Vanni I, Salvadori S, Venditti A, Zhang S,
    Bosman SEI, Bañados E, Davies FB, Fan X, Jun HD, Jin X, Li M, Rojas-Ruiz S, Wang
    F, Yang J, Zou S, Zhang H, Zhu Y. 2026. First-star imprints in a metal-poor galaxy
    overdensity near the end of reionization. Nature Astronomy.
  mla: Li, Zihao, et al. “First-Star Imprints in a Metal-Poor Galaxy Overdensity near
    the End of Reionization.” <i>Nature Astronomy</i>, Springer Nature, 2026, doi:<a
    href="https://doi.org/10.1038/s41550-026-02993-5">10.1038/s41550-026-02993-5</a>.
  short: Z. Li, K. Kakiichi, L. Christensen, Z. Cai, V. D’Odorico, J.J. Matthee, D.
    Kashino, R. Bordoloi, R. Mackenzie, T.A.M. Berg, I. Vanni, S. Salvadori, A. Venditti,
    S. Zhang, S.E.I. Bosman, E. Bañados, F.B. Davies, X. Fan, H.D. Jun, X. Jin, M.
    Li, S. Rojas-Ruiz, F. Wang, J. Yang, S. Zou, H. Zhang, Y. Zhu, Nature Astronomy
    (2026).
das_tickbox: '1'
dataavailabilitystatement: This work is based on observations made with the NASA/ESA/CSA
  JWST, associated with the programmes GO-1243 and GO-2078, and the Very Large Telescope
  associated with ESO programmes X-shooter 0100.A-0625, 0102.A-0154, 1103.A-0817 and
  096.A-0095. The JWST data are available via the Mikulski Archive for Space Telescopes
  at http://archive.stsci.edu under JWST programmes GO-2078 (ref. 127) and GO-1243
  (ref. 128). The metal absorber catalogue of XQR-30 is available via GitHub at https://github.com/XQR-30/Metal-catalogue.
  The [O III] emitter catalogue from the EIGER survey is available via GitHub at https://eiger-jwst.github.io/data.html.
  Other data presented in this paper are available upon request to the corresponding
  author.
date_created: 2026-10-11T22:02:07Z
date_published: 2026-09-29T00:00:00Z
date_updated: 2026-10-14T06:42:17Z
day: '29'
department:
- _id: JoMa
doi: 10.1038/s41550-026-02993-5
fulldoi: https://doi.org/10.1038/s41550-026-02993-5
language:
- iso: eng
month: '09'
oa_version: None
publication: Nature Astronomy
publication_identifier:
  eissn:
  - 2397-3366
publication_status: epub_ahead
publisher: Springer Nature
quality_controlled: '1'
researchdata_availability: yes
scopus_import: '1'
status: public
supplementarymaterial: yes
title: First-star imprints in a metal-poor galaxy overdensity near the end of reionization
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
year: '2026'
...
---
OA_place: repository
OA_type: green
_id: '23112'
abstract:
- lang: eng
  text: We study the joint spectral properties of two coupled random matrices H(1)
    and H(2), which are either real symmetric or complex Hermitian. The entries of
    these matrices exhibit polynomially decaying correlations, both within each matrix
    and between them. Surprisingly, we find that under extremely weak decorrelation
    condition, permitting H(1) and H(2) to be almost fully correlated, the fluctuations
    of their individual eigenvalues in the bulk of the spectrum are still asymptotically
    independent. Furthermore, we demonstrate that this decorrelation condition is
    optimal.
acknowledgement: The author is grateful to László Erdős and Giorgio Cipolloni for
  suggesting the project and fruitful discussions. The author was supported by the
  ERC Advanced Grant “RMTBeyond” No. 101020331.
article_processing_charge: No
article_type: original
arxiv: 1
author:
- first_name: Oleksii
  full_name: Kolupaiev, Oleksii
  id: 149b70d4-896a-11ed-bdf8-8c63fd44ca61
  last_name: Kolupaiev
  orcid: 0000-0003-1491-4623
citation:
  ama: Kolupaiev O. Spectral independence of almost fully correlated random matrices.
    <i>Bernoulli</i>. 2026;32(4):2999-3023. doi:<a href="https://doi.org/10.3150/26-bej1976">10.3150/26-bej1976</a>
  apa: Kolupaiev, O. (2026). Spectral independence of almost fully correlated random
    matrices. <i>Bernoulli</i>. Bernoulli Society for Mathematical Statistics and
    Probability. <a href="https://doi.org/10.3150/26-bej1976">https://doi.org/10.3150/26-bej1976</a>
  chicago: Kolupaiev, Oleksii. “Spectral Independence of Almost Fully Correlated Random
    Matrices.” <i>Bernoulli</i>. Bernoulli Society for Mathematical Statistics and
    Probability, 2026. <a href="https://doi.org/10.3150/26-bej1976">https://doi.org/10.3150/26-bej1976</a>.
  ieee: O. Kolupaiev, “Spectral independence of almost fully correlated random matrices,”
    <i>Bernoulli</i>, vol. 32, no. 4. Bernoulli Society for Mathematical Statistics
    and Probability, pp. 2999–3023, 2026.
  ista: Kolupaiev O. 2026. Spectral independence of almost fully correlated random
    matrices. Bernoulli. 32(4), 2999–3023.
  mla: Kolupaiev, Oleksii. “Spectral Independence of Almost Fully Correlated Random
    Matrices.” <i>Bernoulli</i>, vol. 32, no. 4, Bernoulli Society for Mathematical
    Statistics and Probability, 2026, pp. 2999–3023, doi:<a href="https://doi.org/10.3150/26-bej1976">10.3150/26-bej1976</a>.
  short: O. Kolupaiev, Bernoulli 32 (2026) 2999–3023.
corr_author: '1'
das_tickbox: '0'
date_created: 2026-10-12T12:04:45Z
date_published: 2026-11-01T00:00:00Z
date_updated: 2026-10-14T07:34:08Z
day: '01'
department:
- _id: LaEr
doi: 10.3150/26-bej1976
ec_funded: 1
external_id:
  arxiv:
  - '2503.21472'
fulldoi: https://doi.org/10.3150/26-bej1976
intvolume: '        32'
issue: '4'
keyword:
- correlated random matrix
- eigenvalue perturbation theory
- Local law
- Wigner-type matrix
language:
- iso: eng
main_file_link:
- open_access: '1'
  url: https://doi.org/10.48550/arXiv.2503.21472
month: '11'
oa: 1
oa_version: Preprint
page: 2999-3023
project:
- _id: 62796744-2b32-11ec-9570-940b20777f1d
  call_identifier: H2020
  grant_number: '101020331'
  name: Random matrices beyond Wigner-Dyson-Mehta
publication: Bernoulli
publication_identifier:
  issn:
  - 1350-7265
publication_status: published
publisher: Bernoulli Society for Mathematical Statistics and Probability
quality_controlled: '1'
researchdata_availability: no
scopus_import: '1'
status: public
supplementarymaterial: no
title: Spectral independence of almost fully correlated random matrices
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 32
year: '2026'
...
---
OA_place: publisher
OA_type: free access
_id: '23060'
article_processing_charge: No
article_type: editorial
author:
- first_name: Chiara
  full_name: Ziletti, Chiara
  id: D865714E-FA4E-11E9-B85B-F5C5E5697425
  last_name: Ziletti
citation:
  ama: Ziletti C. International Council on Archives (ICA) Barcelona Congress 2025,
    27-30 October 2025. <i>Scrinium</i>. 2026;80:181-186.
  apa: 'Ziletti, C. (2026). International Council on Archives (ICA) Barcelona Congress
    2025, 27-30 October 2025. <i>Scrinium</i>. Barcelona, Spain: Anton Pustet Verlag.'
  chicago: Ziletti, Chiara. “International Council on Archives (ICA) Barcelona Congress
    2025, 27-30 October 2025.” <i>Scrinium</i>. Anton Pustet Verlag, 2026.
  ieee: C. Ziletti, “International Council on Archives (ICA) Barcelona Congress 2025,
    27-30 October 2025,” <i>Scrinium</i>, vol. 80. Anton Pustet Verlag, pp. 181–186,
    2026.
  ista: Ziletti C. 2026. International Council on Archives (ICA) Barcelona Congress
    2025, 27-30 October 2025. Scrinium. 80, 181–186.
  mla: Ziletti, Chiara. “International Council on Archives (ICA) Barcelona Congress
    2025, 27-30 October 2025.” <i>Scrinium</i>, vol. 80, Anton Pustet Verlag, 2026,
    pp. 181–86.
  short: C. Ziletti, Scrinium 80 (2026) 181–186.
conference:
  end_date: 2025-10-30
  location: Barcelona, Spain
  name: 'ICA: International Council on Archives'
  start_date: 2025-10-27
corr_author: '1'
date_created: 2026-10-05T14:18:42Z
date_published: 2026-10-01T00:00:00Z
date_updated: 2026-10-14T06:56:51Z
day: '01'
ddc:
- '020'
department:
- _id: E-Lib
file:
- access_level: open_access
  checksum: e6fa3953b73e1f900a52a525e82c0685
  content_type: application/pdf
  creator: cziletti
  date_created: 2026-10-12T09:48:09Z
  date_updated: 2026-10-12T09:48:09Z
  file_id: '23106'
  file_name: Scrinium_Ziletti.pdf
  file_size: 555357
  relation: main_file
  success: 1
file_date_updated: 2026-10-12T09:48:09Z
has_accepted_license: '1'
intvolume: '        80'
language:
- iso: eng
month: '10'
oa: 1
oa_version: Published Version
page: 181-186
publication: Scrinium
publication_identifier:
  isbn:
  - '9783702512187'
  issn:
  - 1012-0327
publication_status: published
publisher: Anton Pustet Verlag
status: public
title: International Council on Archives (ICA) Barcelona Congress 2025, 27-30 October
  2025
type: journal_article
user_id: 2DF688A6-F248-11E8-B48F-1D18A9856A87
volume: 80
year: '2026'
...
