@article{18764,
  abstract     = {We prove that a class of weakly perturbed Hamiltonians of the form H_λ= H_0 + λW, with W being a Wigner matrix, exhibits prethermalization. That is, the time evolution generated by H_λ relaxes to its ultimate thermal state via an intermediate prethermal state with a lifetime of order λ^{-2}. Moreover, we obtain a general relaxation formula, expressing the perturbed dynamics via the unperturbed dynamics and the ultimate thermal state. The proof relies on a two-resolvent law for the deformed Wigner matrix H_λ.},
  author       = {Erdös, László and Henheik, Sven Joscha and Reker, Jana and Riabov, Volodymyr},
  issn         = {1424-0637},
  journal      = {Annales Henri Poincare},
  pages        = {1991--2033},
  publisher    = {Springer Nature},
  title        = {{Prethermalization for deformed Wigner matrices}},
  doi          = {10.1007/s00023-024-01518-y},
  volume       = {26},
  year         = {2025},
}

@inbook{18765,
  abstract     = {Mosaic Analysis with Double Markers (MADM) represents a mouse genetic approach coupling differential fluorescent labeling to genetic manipulations in dividing cells and their lineages. MADM uniquely enables the generation and visualization of individual control or homozygous mutant cells in a heterozygous genetic environment. Among its diverse applications, MADM has been used to dissect cell-autonomous gene functions important for cortical development and neural development in general. The high cellular resolution offered by MADM also permits the analysis of transcriptomic changes of individual cells upon genetic manipulations. In this chapter, we describe an experimental protocol combining the generation and isolation of MADM-labeled cells with downstream single-cell RNA-sequencing technologies to probe cell-type specific phenotypes due to genetic mutations at single-cell resolution.},
  author       = {Cheung, Giselle T and Pauler, Florian and Hippenmeyer, Simon},
  booktitle    = {Lineage Tracing},
  editor       = {Garcia-Marques, Jorge and Lee, Tzumin},
  isbn         = {9781071643099},
  issn         = {1940-6029},
  pages        = {139--151},
  publisher    = {Springer Nature},
  title        = {{Probing Cell-Type Specificity of Mutant Phenotype at Transcriptomic Level Using Mosaic Analysis with Double Markers (MADM)}},
  doi          = {10.1007/978-1-0716-4310-5_7},
  volume       = {2886},
  year         = {2025},
}

@article{18778,
  abstract     = {Transcription by RNA polymerase II (Pol II) can be repressed by noncoding RNA, including the human RNA Alu. However, the mechanism by which endogenous RNAs repress transcription remains unclear. Here we present cryogenic-electron microscopy structures of Pol II bound to Alu RNA, which reveal that Alu RNA mimics how DNA and RNA bind to Pol II during transcription elongation. Further, we show how distinct domains of the general transcription factor TFIIF control repressive activity. Together, we reveal how a noncoding RNA can regulate mammalian gene expression.},
  author       = {Tluckova, Katarina and Kaczmarek, Beata M and Testa Salmazo, Anita P and Bernecky, Carrie A},
  issn         = {1545-9985},
  journal      = {Nature Structural & Molecular Biology},
  pages        = {607--612},
  publisher    = {Springer Nature},
  title        = {{Mechanism of mammalian transcriptional repression by noncoding RNA}},
  doi          = {10.1038/s41594-024-01448-7},
  volume       = {32},
  year         = {2025},
}

@article{18807,
  abstract     = {Developing tissues interpret dynamic changes in morphogen activity to generate cell type diversity. To quantitatively study bone morphogenetic protein (BMP) signaling dynamics in the mouse neural tube, we developed an embryonic stem cell differentiation system tailored for growing tissues. Differentiating cells form striking self-organized patterns of dorsal neural tube cell types driven by sequential phases of BMP signaling that are observed both in vitro and in vivo. Data-driven biophysical modeling showed that these dynamics result from coupling fast negative feedback with slow positive regulation of signaling by the specification of an endogenous BMP source. Thus, in contrast to relays that propagate morphogen signaling in space, we identify a BMP signaling relay that operates in time. This mechanism allows for a rapid initial concentration-sensitive response that is robustly terminated, thereby regulating balanced sequential cell type generation. Our study provides an experimental and theoretical framework to understand how signaling dynamics are exploited in developing tissues.},
  author       = {Rus, Stefanie and Brückner, David and Minchington, Thomas and Greunz, Martina and Merrin, Jack and Hannezo, Edouard B and Kicheva, Anna},
  issn         = {1534-5807},
  journal      = {Developmental Cell},
  number       = {4},
  pages        = {567--580},
  publisher    = {Elsevier},
  title        = {{Self-organized pattern formation in the developing mouse neural tube by a temporal relay of BMP signaling}},
  doi          = {10.1016/j.devcel.2024.10.024},
  volume       = {60},
  year         = {2025},
}

@article{18820,
  abstract     = {Feature selection is essential in the analysis of molecular systems and many other fields, but several uncertainties remain: What is the optimal number of features for a simplified, interpretable model that retains essential information? How should features with different units be aligned, and how should their relative importance be weighted? Here, we introduce the Differentiable Information Imbalance (DII), an automated method to rank information content between sets of features. Using distances in a ground truth feature space, DII identifies a low-dimensional subset of features that best preserves these relationships. Each feature is scaled by a weight, which is optimized by minimizing the DII through gradient descent. This allows simultaneously performing unit alignment and relative importance scaling, while preserving interpretability. DII can also produce sparse solutions and determine the optimal size of the reduced feature space. We demonstrate the usefulness of this approach on two benchmark molecular problems: (1) identifying collective variables that describe conformations of a biomolecule, and (2) selecting features for training a machine-learning force field. These results show the potential of DII in addressing feature selection challenges and optimizing dimensionality in various applications. The method is available in the Python library DADApy.},
  author       = {Wild, Romina and Wodaczek, Felix and Del Tatto, Vittorio and Cheng, Bingqing and Laio, Alessandro},
  issn         = {2041-1723},
  journal      = {Nature Communications},
  publisher    = {Springer Nature},
  title        = {{Automatic feature selection and weighting in molecular systems using Differentiable Information Imbalance}},
  doi          = {10.1038/s41467-024-55449-7},
  volume       = {16},
  year         = {2025},
}

@article{18821,
  abstract     = {Even though the one-dimensional contact interaction requires no regularization, renormalization methods have been shown to improve the convergence of numerical calculations considerably. In this work, we compare and contrast these methods: “the running coupling constant” where the two-body ground-state energy is used as a renormalization condition, and two effective interaction approaches that include information about the ground as well as excited states. In particular, we calculate the energies and densities of few-fermion systems in a harmonic oscillator with the configuration-interaction method and compare the results based upon renormalized and bare interactions. We find that the use of the running coupling constant instead of the bare interaction improves convergence significantly. A comparison with an effective interaction, which is designed to reproduce the relative part of the energy spectrum of two particles, showed a similar improvement. The effective interaction provides an additional improvement if the center-of-mass excitations are included in the construction. Finally, we discuss the transformation of observables alongside the renormalization of the potential, and demonstrate that this might be an essential ingredient for accurate numerical calculations.},
  author       = {Brauneis, Fabian and Hammer, Hans Werner and Reimann, Stephanie M. and Volosniev, Artem},
  issn         = {2469-9934},
  journal      = {Physical Review A},
  number       = {1},
  publisher    = {American Physical Society},
  title        = {{Comparison of renormalized interactions using one-dimensional few-body systems as a testbed}},
  doi          = {10.1103/PhysRevA.111.013303},
  volume       = {111},
  year         = {2025},
}

@article{18822,
  abstract     = {Let N(X) be the number of integral zeros (mathematical equation). Works of Hooley and Heath-Brown imply (mathematical equation), if one assumes automorphy and grand Riemann hypothesis for certain Hasse–Weil L-functions. Assuming instead a natural large sieve inequality, we recover the same bound on N(X). This is part of a more general statement, for diagonal cubic forms in (mathematical equation) variables, where we allow approximations to Hasse–Weil L-functions.},
  author       = {Wang, Victor},
  issn         = {2041-7942},
  journal      = {Mathematika},
  number       = {1},
  publisher    = {London Mathematical Society},
  title        = {{Diagonal cubic forms and the large sieve}},
  doi          = {10.1112/mtk.70008},
  volume       = {71},
  year         = {2025},
}

@article{18823,
  author       = {Cao, Dechang and De Jaeger-Braet, Joke G},
  issn         = {1532-2548},
  journal      = {Plant Physiology},
  number       = {1},
  publisher    = {Oxford University Press},
  title        = {{Memory of maternal temperatures: DNA methylation alterations across generations}},
  doi          = {10.1093/plphys/kiae651},
  volume       = {197},
  year         = {2025},
}

@misc{18837,
  abstract     = {Super-resolution methods provide far better spatial resolution than the optical diffraction limit of about half the wavelength of light (∼200-300 nm). Nevertheless, they have yet to attain widespread use in plants, largely due to plants’ challenging optical properties. Expansion microscopy improves effective resolution by isotropically increasing the physical distances between sample structures while preserving relative spatial arrangements and clearing the sample. However, its application to plants has been hindered by the rigid, mechanically cohesive structure of plant tissues. Here, we report on whole-mount expansion microscopy of thale cress (Arabidopsis thaliana) root tissues (PlantEx), achieving a four-fold resolution increase over conventional microscopy. Our results highlight the microtubule cytoskeleton organization and interaction between molecularly defined cellular constituents. Combining PlantEx with stimulated emission depletion (STED) microscopy, we increase nanoscale resolution and visualize the complex organization of subcellular organelles from intact tissues by example of the densely packed COPI-coated vesicles associated with the Golgi apparatus and put these into a cellular structural context. Our results show that expansion microscopy can be applied to increase effective imaging resolution in Arabidopsis root specimens.},
  author       = {Danzl, Johann G and Kreuzinger, Caroline},
  publisher    = {Institute of Science and Technology Austria},
  title        = {{Research Data for the publication "Super-resolution expansion microscopy in plant roots"}},
  doi          = {10.15479/AT:ISTA:18837},
  year         = {2025},
}

@article{18848,
  abstract     = {Type II CRISPR endonucleases are widely used programmable genome editing tools. Recently, CRISPR-Cas systems with highly compact nucleases have been discovered, including Cas9d (a type II-D nuclease). Here, we report the cryo-EM structures of a Cas9d nuclease (747 amino acids in length) in multiple functional states, revealing a stepwise process of DNA targeting involving a conformational switch in a REC2 domain insertion. Our structures provide insights into the intricately folded guide RNA which acts as a structural scaffold to anchor small, flexible protein domains for DNA recognition. The sgRNA can be truncated by up to ~25% yet still retain activity in vivo. Using ancestral sequence reconstruction, we generated compact nucleases capable of efficient genome editing in mammalian cells. Collectively, our results provide mechanistic insights into the evolution and DNA targeting of diverse type II CRISPR-Cas systems, providing a blueprint for future re-engineering of minimal RNA-guided DNA endonucleases.},
  author       = {Ocampo, Rodrigo Fregoso and Bravo, Jack Peter Kelly and Dangerfield, Tyler L. and Nocedal, Isabel and Jirde, Samatar A. and Alexander, Lisa M. and Thomas, Nicole C. and Das, Anjali and Nielson, Sarah and Johnson, Kenneth A. and Brown, Christopher T. and Butterfield, Cristina N. and Goltsman, Daniela S.A. and Taylor, David W.},
  issn         = {2041-1723},
  journal      = {Nature Communications},
  publisher    = {Springer Nature},
  title        = {{DNA targeting by compact Cas9d and its resurrected ancestor}},
  doi          = {10.1038/s41467-024-55573-4},
  volume       = {16},
  year         = {2025},
}

@article{18849,
  abstract     = {Many biological systems operate near the physical limits to their performance, suggesting that aspects of their behavior and underlying mechanisms could be derived from optimization principles. However, such principles have often been applied only in simplified models. Here, we explore a detailed mechanistic model of the gap gene network in the Drosophila embryo, optimizing its 50+ parameters to maximize the information that gene expression levels provide about nuclear positions. This optimization is conducted under realistic constraints, such as limits on the number of available molecules. Remarkably, the optimal networks we derive closely match the architecture and spatial gene expression profiles observed in the real organism. Our framework quantifies the tradeoffs involved in maximizing functional performance and allows for the exploration of alternative network configurations, addressing the question of which features are necessary and which are contingent. Our results suggest that multiple solutions to the optimization problem might exist across closely related organisms, offering insights into the evolution of gene regulatory networks.},
  author       = {Sokolowski, Thomas R and Gregor, Thomas and Bialek, William and Tkačik, Gašper},
  issn         = {1091-6490},
  journal      = {Proceedings of the National Academy of Sciences},
  number       = {1},
  publisher    = {National Academy of Sciences},
  title        = {{Deriving a genetic regulatory network from an optimization principle}},
  doi          = {10.1073/pnas.2402925121},
  volume       = {122},
  year         = {2025},
}

@article{18850,
  abstract     = {Biophysical constraints limit the specificity with which transcription factors (TFs) can target regulatory DNA. While individual nontarget binding events may be low affinity, the sheer number of such interactions could present a challenge for gene regulation by degrading its precision or possibly leading to an erroneous induction state. Chromatin can prevent nontarget binding by rendering DNA physically inaccessible to TFs, at the cost of energy-consuming remodeling orchestrated by pioneer factors (PFs). Under what conditions and by how much can chromatin reduce regulatory errors on a global scale? We use a theoretical approach to compare two scenarios for gene regulation: one that relies on TF binding to free DNA alone and one that uses a combination of TFs and chromatin-regulating PFs to achieve desired gene expression patterns. We find, first, that chromatin effectively silences groups of genes that should be simultaneously OFF, thereby allowing more accurate graded control of expression for the remaining ON genes. Second, chromatin buffers the deleterious consequences of nontarget binding as the number of OFF genes grows, permitting a substantial expansion in regulatory complexity. Third, chromatin-based regulation productively co-opts nontarget TF binding for ON genes in order to establish a “leaky” baseline expression level, which targeted activator or repressor binding subsequently up- or down-modulates. Thus, on a global scale, using chromatin simultaneously alleviates pressure for high specificity of regulatory interactions and enables an increase in genome size with minimal impact on global expression error.},
  author       = {Perkins, Mindy Liu and Crocker, Justin and Tkačik, Gašper},
  issn         = {1091-6490},
  journal      = {Proceedings of the National Academy of Sciences},
  number       = {1},
  publisher    = {National Academy of Sciences},
  title        = {{Chromatin enables precise and scalable gene regulation with factors of limited specificity}},
  doi          = {10.1073/pnas.2411887121},
  volume       = {122},
  year         = {2025},
}

@article{18851,
  abstract     = {We present volume-limited samples of cataclysmic variables (CVs) and AM CVn binaries jointly selected from SRG/eROSITA eRASS1 and Gaia DR3 using an X-ray + optical color–color diagram (the "X-ray Main Sequence"). This tool identifies all CV subtypes, including magnetic and low-accretion rate systems, in contrast to most previous surveys. We find 23 CVs, 3 of which are AM CVns, out to 150 pc in the Western Galactic Hemisphere. Our 150 pc sample is spectroscopically verified and complete down to LX = 1.3 × 1029 erg s−1 in the 0.2–2.3 keV band, and we also present CV candidates out to 300 pc and 1000 pc. We discovered two previously unknown systems in our 150 pc sample: the third nearest AM CVn and a magnetic period bouncer. We find the mean LX of CVs to be 〈LX〉 ≈ 4.6 × 1030 erg s−1, in contrast to previous surveys which yielded 〈LX〉 ∼ 1031−1032 erg s−1. We construct X-ray luminosity functions that, for the first time, flatten out at LX ∼ 1030 erg s−1. We infer average number, mass, and luminosity densities of ρN,CV = (3.7 ± 0.7) × 10−6pc−3, (math formular), and (math formular), respectively, in the solar neighborhood. Our uniform selection method also allows us to place meaningful estimates on the space density of AM CVns, ρN,AM CVn = (5.5 ± 3.7) × 10−7 pc−3. Magnetic CVs and period bouncers make up 35% and 25% of our sample, respectively. This work, through a novel discovery technique, shows that the observed number densities of CVs and AM CVns, as well as the fraction of period bouncers, are still in tension with population synthesis estimates.},
  author       = {Rodriguez, Antonio C. and El-Badry, Kareem and Suleimanov, Valery and Pala, Anna F. and Kulkarni, Shrinivas R. and Gaensicke, Boris and Mori, Kaya and Rich, R. Michael and Sarkar, Arnab and Bao, Tong and De Oliveira, Raimundo Lopes and Ramsay, Gavin and Szkody, Paula and Graham, Matthew and Prince, Thomas A. and Caiazzo, Ilaria and Vanderbosch, Zachary P. and Roestel, Jan Van and Das, Kaustav K. and Qin, Yu Jing and Kasliwal, Mansi M. and Wold, Avery and Groom, Steven L. and Reiley, Daniel and Riddle, Reed},
  issn         = {0004-6280},
  journal      = {Publications of the Astronomical Society of the Pacific},
  number       = {1},
  publisher    = {IOP Publishing},
  title        = {{Cataclysmic variables and AM CVn binaries in SRG/eROSITA + Gaia: Volume limited samples, X-ray luminosity functions, and space densities}},
  doi          = {10.1088/1538-3873/ada185},
  volume       = {137},
  year         = {2025},
}

@article{18852,
  abstract     = {Recent observations have found a growing number of hypervelocity stars with speeds of ≈1500 − 2500 km s−1 that could have only been produced through thermonuclear supernovae in white dwarf binaries. Most of the observed hypervelocity runaways in this class display a surprising inflated structure: their current radii are roughly an order of magnitude greater than they would have been as white dwarfs filling their Roche lobe. While many simulations exist studying the dynamical phase leading to supernova detonation in these systems, no detailed calculations of the long-term structure of the runaways have yet been performed. We used an existing AREPO hydrodynamical simulation of a supernova in a white dwarf binary as a starting point for the evolution of these stars with the one-dimensional stellar evolution code MESA. We show that the supernova shock is not energetic enough to inflate the white dwarf over timescales longer than a few thousand years, significantly shorter than the 105 − 6 year lifetimes inferred for observed hypervelocity runaways. Although they experience a shock from a supernova less than ≈0.02 R⊙ away, our models do not experience significant interior heating, and all contract back to radii of around 0.01 R⊙ within about 104 years. Explaining the observed inflated states requires either an additional source of significant heating or some other physics that is not yet accounted for in the subsequent evolution.},
  author       = {Bhat, Aakash and Bauer, Evan B. and Pakmor, Rüdiger and Shen, Ken J. and Caiazzo, Ilaria and Rajamuthukumar, Abinaya Swaruba and El-Badry, Kareem and Kerzendorf, Wolfgang E.},
  issn         = {1432-0746},
  journal      = {Astronomy & Astrophysics},
  number       = {1},
  publisher    = {EDP Sciences},
  title        = {{Supernova shocks cannot explain the inflated state of hypervelocity runaways from white dwarf binaries}},
  doi          = {10.1051/0004-6361/202451371},
  volume       = {693},
  year         = {2025},
}

@article{18853,
  abstract     = {Electrolyte additives are extensively validated effective in mitigating dendrite growth and parasitic reactions in aqueous zinc-ion batteries (AZIBs). Nonetheless, the mechanisms by which additives influence the formation and characteristics of the inorganic solid–electrolyte interphase (SEI) are not yet fully elucidated. Herein, we investigate how Zn(CF3COO)2 additives influence solvation structure and elucidate the mechanism by which these additives promote the dual reduction of anions. Through cryo-transmission electron microscopy analysis, we identified the SEI as a highly amorphous ZnS/ZnF2 phase. This amorphous hybrid SEI demonstrates exceptional stability, mechanical robustness, and high Zn2+ conductivity, effectively mitigating parasitic reactions and enhancing Zn plating/stripping reversibility. Even under elevated current densities, the Zn anode exhibits ultra-stable longevity and ultra-high reversibility. This study provides a comprehensive understanding of the intrinsic mechanisms governing solvation structure modulation that lead to the formation of amorphous hybrid SEI, underscoring their efficacy in enhancing the performance and durability of AZIBs.},
  author       = {Zeng, Guifang and Sun, Qing and Horta, Sharona and Martínez-Alanis, Paulina R. and Wu, Peng and Li, Jing and Wang, Shang and Ibáñez, Maria and Tian, Yanhong and Ci, Lijie and Cabot, Andreu},
  issn         = {1754-5706},
  journal      = {Energy and Environmental Science},
  number       = {4},
  pages        = {1683--1695},
  publisher    = {Royal Society of Chemistry},
  title        = {{Modulating the solvation structure to enhance amorphous solid electrolyte interface formation for ultra-stable aqueous zinc anode}},
  doi          = {10.1039/d4ee03750b},
  volume       = {18},
  year         = {2025},
}

@article{18854,
  abstract     = {Context. One of the surprising early findings with JWST has been the discovery of a strong “roll-over” or a softening of the absorption edge of Lyα in a large number of galaxies at z ≳ 6, in addition to systematic offsets from photometric redshift estimates and fundamental galaxy scaling relations. This has been interpreted as strong cumulative damped Lyα absorption (DLA) wings from high column densities of neutral atomic hydrogen (H I), signifying major gas accretion events in the formation of these galaxies.
Aims. To explore this new phenomenon systematically, we assembled the JWST/NIRSpec PRImordial gas Mass AssembLy (PRIMAL) legacy survey of 584 galaxies at z = 5.0 − 13.4, designed to study the physical properties and gas in and around galaxies during the reionization epoch.
Methods. We characterized this benchmark sample in full and spectroscopically derived the galaxy redshifts, metallicities, star formation rates, and ultraviolet (UV) slopes. We defined a new diagnostic, the Lyα damping parameter DLyα, to measure and quantify the net effect of Lyα emission strength, the H I fraction in the intergalactic medium, or the local H I column density for each source. The JWST-PRIMAL survey is based on the spectroscopic DAWN JWST Archive (DJA-Spec). We describe DJA-Spec in this paper, detailing the reduction methods, the post-processing steps, and basic analysis tools. All the software, reduced spectra, and spectroscopically derived quantities and catalogs are made publicly available in dedicated repositories.
Results. We find that the fraction of galaxies showing strong integrated DLAs with NHI > 1021 cm−2 only increases slightly from ≈60% at z ≈ 6 up to ≈65 − 90% at z > 8. Similarly, the prevalence and prominence of Lyα emission is found to increase with decreasing redshift, in qualitative agreement with previous observational results. Strong Lyα emitters (LAEs) are predominantly found to be associated with low-metallicity and UV faint galaxies. By contrast, strong DLAs are observed in galaxies with a variety of intrinsic physical properties, but predominantly at high redshifts and low metallicities.
Conclusions. Our results indicate that strong DLAs likely reflect a particular early assembly phase of reionization-era galaxies, at which point they are largely dominated by pristine H I gas accretion. At z = 8 − 10, this gas gradually cools and forms into stars that ionize their local surroundings, forming large ionized bubbles and producing strong observed Lyα emission at z < 8.},
  author       = {Heintz, K. E. and Brammer, G. B. and Watson, D. and Oesch, P. A. and Keating, L. C. and Hayes, M. J. and Abdurro'Uf, Unknown and Arellano-Córdova, K. Z. and Carnall, A. C. and Christiansen, C. R. and Cullen, F. and Davé, R. and Dayal, P. and Ferrara, A. and Finlator, K. and Fynbo, J. P.U. and Flury, S. R. and Gelli, V. and Gillman, S. and Gottumukkala, R. and Gould, K. and Greve, T. R. and Hardin, S. E. and Hsiao, T. Y.Y. and Hutter, A. and Jakobsson, P. and Killi, M. and Khosravaninezhad, N. and Laursen, P. and Lee, M. M. and Magdis, G. E. and Matthee, Jorryt J and Naidu, R. P. and Narayanan, D. and Pollock, C. and Prescott, M. K.M. and Rusakov, V. and Shuntov, M. and Sneppen, A. and Smit, R. and Tanvir, N. R. and Terp, C. and Toft, S. and Valentino, F. and Vijayan, A. P. and Weaver, J. R. and Wise, J. H. and Witstok, J.},
  issn         = {1432-0746},
  journal      = {Astronomy & Astrophysics},
  publisher    = {EDP Sciences},
  title        = {{The JWST-PRIMAL archival survey: A JWST/NIRSpec reference sample for the physical properties and Lyman-α absorption and emission of ∼600 galaxies at z = 5.0-13.4}},
  doi          = {10.1051/0004-6361/202450243},
  volume       = {693},
  year         = {2025},
}

@article{18855,
  abstract     = {A central problem in computational statistics is to convert a procedure for sampling combinatorial objects into a procedure for counting those objects, and vice versa. We consider sampling problems which come from Gibbs distributions, which are families of probability distributions over a discrete space Ω with probability mass function of the form μ^Ω_β(ω) ∝ e^{β H(ω)} for β in an interval [β_min, β_max] and H(ω) ∈ {0} ∪ [1, n]. Two important parameters are the partition function, which is the normalization factor Z(β) = ∑_{ω ∈ Ω} e^{β H(ω)}, and the vector of pre-image counts c_x=|H^-1(x)|.
We develop black-box sampling algorithms to estimate the counts roughly Õ(n²/ε²) samples for integer-valued distributions and Õ(q/ε²) samples for general distributions, where q = (log Z(β_max))/Z(β_min)  (ignoring some second-order terms and parameters). We show this is optimal up to logarithmic factors. We illustrate with improved algorithms for counting connected subgraphs, independent sets, and perfect matchings. As a key subroutine, we estimate all values of the partition function using Õ(n²/ε²) samples for integer-valued distributions and Õ(q/ε²) samples for general distributions. This improves over a prior algorithm of Huber (2015) which computes a single point estimate Z(β_max) and which uses a slightly larger amount of samples. We show matching lower bounds, demonstrating this complexity is optimal as a function of n and q up to logarithmic terms.},
  author       = {Harris, David G. and Kolmogorov, Vladimir},
  issn         = {1549-6333},
  journal      = {ACM Transactions on Algorithms},
  number       = {1},
  publisher    = {Association for Computing Machinery},
  title        = {{Parameter estimation for Gibbs distributions}},
  doi          = {10.1145/3685676},
  volume       = {21},
  year         = {2025},
}

@article{18866,
  abstract     = {Using JWST Near Infrared Camera (NIRCam) images of the globular cluster 47,Tucanæ, (or NGC,104), taken at two epochs just 7 months apart, we derived proper-motion membership down to F322W2 ∼ 27. We identified an intriguing feature at the very low-mass end of the main sequence, around ∼ 0.08,M_⋅, at magnitudes F322W2 ∼ 24 and m_ F150W2 ∼ 25. This feature, dubbed 'kink', is characterized by a prominent discontinuity in the slope of the main sequence. A similar discontinuity is seen in theoretical isochrones with oxygen-poor chemistries, related to the rapid onset of absorption. We therefore hypothesize that the cluster hosts disproportionately more oxygen-poor stars near the bottom of the main sequence compared to the upper main sequence and the red giant branch. Our results show no strong or conclusive evidence of a rise in the brown dwarf luminosity function at faint magnitudes, in contrast to previous findings likely affected by faint red background galaxies. In our analysis, we accounted for this contamination by using proper motion membership.},
  author       = {Scalco, M. and Gerasimov, R. and Bedin, L. R. and Vesperini, E. and Correnti, M. and Nardiello, D. and Burgasser, A. and Richer, H. and Caiazzo, Ilaria and Heyl, J. and Libralato, M. and Anderson, J. and Griggio, M.},
  issn         = {1432-0746},
  journal      = {Astronomy & Astrophysics},
  publisher    = {EDP Sciences},
  title        = {{JWST photometry and astrometry of 47 Tucanae. Discontinuity in the stellar sequence at the star--brown dwarf transition}},
  doi          = {10.1051/0004-6361/202452907},
  volume       = {694},
  year         = {2025},
}

@phdthesis{18871,
  abstract     = {"Can we do this with a new type of computer - a quantum computer?". This famous
quotation of the brilliant Richard Feynman within a conference talk on "Simulating physics
with computers.” is often reverently praised as the origin of the field of quantum computing.
The idea was to use quantum mechanical systems itself to simulate "Nature", which is
inherently quantum mechanical. Now, 43 years later, the theoretical framework of how such
a computer can operate has been developed. Two main important concepts for a potential
quantum supremacy, superposition and entanglement, have been exploited to design quantum
algorithms to significantly speed up certain tasks. Yet, the specific hardware implementation
is still far from being certain, in fact the race between the most promising platforms such as
superconducting qubits, bosonic codes, cold atoms, trapped ions, optical computing as well
as spin qubits has recently intensified. If one also includes the most mature applications of
quantum communication technologies, secure quantum key distribution and quantum random
number generators, as part of a quantum information technology ecosystem, we are confronted
with a plethora of different materials, concepts, and also operation frequencies. While
superconducting qubits, bosonic codes and spin qubits work in the regime of approximately 5
GHz and are controlled by electrical fields, trapped ions, cold atoms, and optical quantum
computing operate with light in the infrared or visible range.
Consequently, a quantum frequency converter or microwave-optic transducer is required
to interface the different frequency domains or establish a long-range network connection
with suitable telecom fibers. In fact, the combination of different frequency regimes is also
an essential part in our classical modern communication network, where computations are
performed in electrical circuits and the information exchange over longer distances happens
via optical fibers. However, the specific challenges specific to building a quantum computer,
also apply to the development of such a quantum frequency transducer: 1) As we deal with
single excitations as the carrier of information, i.e. the smallest possible quantity, the signal
can easily be corrupted by other noise sources which needs to be avoided by all means. This
is also the reason why microwave quantum computers operate at temperature environments
close to zero temperature (< 0.1 Kelvin) to avoid corruption by thermal noise. 2) The
frequency interface generally needs to preserve the phase of the signal as an essential part
of the quantum state. And 3) Quantum signals cannot be copied which would be a typical
strategy to account for errors in classical computers. And finally, there is a challenge specific to
microwave-optic transducers: While quantum computers are operating in one specific frequency
domain, microwave-optic transducers combine microwave and optical fields in one device.
This results in the particular challenge that high-energy optical radiation, which is usually
well-shielded from superconducting microwave quantum processors, are now an essential part
of the device. The concomitant optical radiation in the operating transducer will inevitably
have a detrimental effect on the superconducting microwave components. Together with the
requirement of minimal background noise for quantum-limited operation as described above,
v
heating from the absorption of optical photons within the same device where single microwave
excitations are processed forms a formidable challenge.
This thesis aims to address this challenge by developing microwave-optic transducers where
the impact of optical absorption on superconducting circuits in general and superconducting
qubits specifically can be mitigated. In our first approach, we developed a compact device
with optimized interaction strengths between the different frequency domains. This minimizes
the optical powers used for transducer operation and thus the optical absorption heating. This
work was - to the best of our knowledge - the first comprehensive noise study, in an integrated
microwave-optic transducer. Unfortunately, we saw that the optical absorption heating added
noise way above a single excitation. Consequently, a potential quantum signal would have
been buried in the noise, added by the transduction.
Building on this insight, we utilized a three-dimensional microwave-optic transducer instead
of an integrated device. The larger heat capacity of the macroscopic device with a size
of a few millimeters can absorb a larger fraction of the optical heating before it increases
the temperature of the device. This allowed us to interface the transducer directly with a
superconducting qubit to readout the qubit state in a novel all-optical manner. We showed
that the microwave-optic transducer can be operated in a regime in which optical fields don’t
harm the sensitive qubit. This is an important prerequisite for the operation of microwave-optic
transducers in conjunction with microwave quantum processors and brings the integration and
seamless orchestration of different frequency components in a quantum network a step closer.
},
  author       = {Arnold, Georg M},
  issn         = {2663-337X},
  pages        = {135},
  publisher    = {Institute of Science and Technology Austria},
  title        = {{Microwave-optic interconnects for superconducting circuits}},
  doi          = {10.15479/at:ista:18871},
  year         = {2025},
}

@article{18878,
  abstract     = {Thermoelectric (TE) materials, with the ability to convert heat into electrical energy, can generate micro-electrical fields at electronic interfaces with biological systems, making them applicable in electric-catalyzing as nanozymes, and modulate the infected microenvironment of skin wounds. Thereby, by harnessing temperature differences in vitro or in vivo, TE nanomaterials can provide antimicrobial reactive oxygen species (ROS) by catalyzing redox reactions, thereby accelerating wound healing by suppressing infection. However, despite their promising potential, there is still a lack of comprehensive understanding of the antimicrobial mechanisms, biocompatibility, and practical applications of TE nanomaterials in wound healing, as this is a newly-emerged sub-area of energy-related biomedical applications. This review aims to address this gap by highlighting the emerging progress of TE materials in wound healing, clarifying their mechanism and advances, emphasizing their potential challenges for commercialization and clinical use, and proposing novel design strategies of TE nanomaterials for effective antibacterial performance.},
  author       = {Jia, Shiyu and Qi, Cai and Xu, Shengduo and Yang, Lei and Sun, Qiang},
  issn         = {1005-0302},
  journal      = {Journal of Materials Science and Technology},
  number       = {08},
  pages        = {212--226},
  publisher    = {Elsevier},
  title        = {{Advancements of thermoelectric nanomaterials in ROS-mediated broad-spectrum antibacterial therapies for wound healing}},
  doi          = {10.1016/j.jmst.2024.11.039},
  volume       = {225},
  year         = {2025},
}

