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Modified Teukolsky formalism: Null testing and numerical benchmarking. Fawzi Aly et. al. https://arxiv.org/abs/2603.01456

11.03.2026 00:48 👍 0 🔁 0 💬 0 📌 0
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Using thermodynamics to learn gravitational wave physics. Caio César Rodrigues Evangelista et. al. https://arxiv.org/abs/2602.21261

11.03.2026 00:48 👍 0 🔁 0 💬 0 📌 0
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Kinetic Route to Helicity-Constrained Decay. Dion Li https://arxiv.org/abs/2602.17514

11.03.2026 00:48 👍 0 🔁 0 💬 0 📌 0
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New solution to the hyperon puzzle of neutron stars: Quantum many-body effects. Hao-Fu Zhu et. al. https://arxiv.org/abs/2602.07939

11.03.2026 00:47 👍 0 🔁 0 💬 0 📌 0
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{Realisation of the MBH binary signals observed over 4 years in LISA. Here we consider $ $ sources (thin black lines). Their total power results from the addition of individual GWs with differing phases (shown are the actual sum and the sum in quadrature, blue lines). The residuals computed with ...

{Realisation of the MBH binary signals observed over 4 years in LISA. Here we consider $ $ sources (thin black lines). Their total power results from the addition of individual GWs with differing phases (shown are the actual sum and the sum in quadrature, blue lines). The residuals computed with ...

Top panel: Residuals calculated from $10^3$ draws from the representative population distributions discussed in section  {sec:Methods:pop

Top panel: Residuals calculated from $10^3$ draws from the representative population distributions discussed in section {sec:Methods:pop

Limits of vacuum-template subtraction for LISA massive black hole binary sources in realistic environments. Lorenz Zwick https://arxiv.org/abs/2601.06684

11.03.2026 00:46 👍 0 🔁 0 💬 0 📌 0
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Kerr-Newman-de Sitter black holes in $f(R)$ gravity with constant curvature: horizon structure and extremality. Alikram N. Aliev et. al. https://arxiv.org/abs/2601.06661

11.03.2026 00:45 👍 0 🔁 0 💬 0 📌 0
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Gravitational Noether-Ward identities for scalar field. Tomislav Prokopec https://arxiv.org/abs/2512.22958

11.03.2026 00:44 👍 1 🔁 0 💬 0 📌 0

Apparent Phantom Crossing in Gauss-Bonnet Gravity. Shin'ichi Nojiri et. al. https://arxiv.org/abs/2512.06279

11.03.2026 00:44 👍 0 🔁 0 💬 0 📌 0
$  ^{CC

$ ^{CC

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: angular resolution in direction reconstruction for ORCA6 (dark purple) and ORCA115 (light purple). Right: $ $ of ratio between reconstructed and true energy. Comparison to a MLF reconstruction algorithm is also shown in orange color.

: angular resolution in direction reconstruction for ORCA6 (dark purple) and ORCA115 (light purple). Right: $ $ of ratio between reconstructed and true energy. Comparison to a MLF reconstruction algorithm is also shown in orange color.

$  ^{CC

$ ^{CC

Enhancing low energy reconstruction and classification in KM3NeT/ORCA with transformers. Iván Mozún Mateo (on behalf of the KM3NeT collaboration) https://arxiv.org/abs/2511.18999

11.03.2026 00:43 👍 0 🔁 0 💬 0 📌 0
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-law GWB model parameters $( {10

-law GWB model parameters $( {10

\% credibility upper limit on $ {

\% credibility upper limit on $ {

Constraining the gravitational-wave emission of core-collapse supernovae with ground-based detectors. Jingwang Diao et. al. https://arxiv.org/abs/2510.23829

11.03.2026 00:42 👍 0 🔁 0 💬 0 📌 0

Scattering of non-relativistic finite-size particles and puffy dark matter direct detection. Wu-Long Xu et. al. https://arxiv.org/abs/2510.10641

11.03.2026 00:41 👍 0 🔁 0 💬 0 📌 1
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Novel very-high-frequency quasi-periodic oscillations of compact, non-singular objects. Jens Boos et. al. https://arxiv.org/abs/2510.00986

11.03.2026 00:41 👍 0 🔁 0 💬 0 📌 0

Cosmological Perturbation in New General Relativity: Propagating mode from the violation of local Lorentz invariance. Kyosuke Tomonari et. al. https://arxiv.org/abs/2509.18772

11.03.2026 00:40 👍 0 🔁 0 💬 0 📌 0
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Incorporating curved geometry in cosmological simulations. Julian Adamek et. al. https://arxiv.org/abs/2508.20606

11.03.2026 00:39 👍 0 🔁 0 💬 0 📌 0
‑Newtonian potentials with $N_1=7$ (purple line) and $N_1=1$ (turquoise line), constructed using the constraints presented in sections   {sec:ISCO

‑Newtonian potentials with $N_1=7$ (purple line) and $N_1=1$ (turquoise line), constructed using the constraints presented in sections {sec:ISCO

‑Newtonian potentials with $N_1=7$ (purple line) and $N_1=1$ (turquoise line), constructed using the constraints presented in sections   {sec:ISCO

‑Newtonian potentials with $N_1=7$ (purple line) and $N_1=1$ (turquoise line), constructed using the constraints presented in sections {sec:ISCO

General form for Pseudo-Newtonian Potentials, imitating Schwarzschild geodesics. Itamar Ben Arosh Arad et. al. https://arxiv.org/abs/2507.15107

11.03.2026 00:39 👍 0 🔁 0 💬 0 📌 0
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Simultaneously search for multi-target Galactic binary gravitational waves. Pin Gao et. al. https://arxiv.org/abs/2401.09300

11.03.2026 00:38 👍 0 🔁 0 💬 0 📌 0
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Explainable classification of astronomical uncertain time series. Michael Franklin Mbouopda (LIMOS et. al. https://arxiv.org/abs/2210.00869

11.03.2026 00:37 👍 0 🔁 0 💬 0 📌 0
IRAC color–color diagram of the MIR sources. The small gray dots represent all IRAC sources selected in the COSMOS. The region bounded by dashed red lines marks the MIR-AGN selection region of  {2012ApJ...748..142D

IRAC color–color diagram of the MIR sources. The small gray dots represent all IRAC sources selected in the COSMOS. The region bounded by dashed red lines marks the MIR-AGN selection region of {2012ApJ...748..142D

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Identifying Compton-thick active galactic nuclei in the COSMOS. II. Searching among mid-infrared selected AGNs. Xiaotong Guo et. al. https://arxiv.org/abs/2603.01453

11.03.2026 00:36 👍 0 🔁 0 💬 0 📌 0
Hess diagrams for the {

Hess diagrams for the {

left panel: the color-magnitude diagram of the 100 pc white dwarf population classified into DA and non-DA by    {JE2023

left panel: the color-magnitude diagram of the 100 pc white dwarf population classified into DA and non-DA by {JE2023

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WDLFs in the $9<M_G<11.5$ range for different values of $g_{ae

WDLFs in the $9<M_G<11.5$ range for different values of $g_{ae

New axion bounds derived from the 100-parsec Gaia DR3 white dwarf luminosity function. Martín L. Alberino et. al. https://arxiv.org/abs/2603.00901

11.03.2026 00:36 👍 0 🔁 0 💬 0 📌 0
$M$--$R$ curves for four externally validated EoSs with NN=valid and TOV=valid.      Solid curves correspond to full TOV integrations, while the NICER credible regions for      PSR~J0030 and PSR~J0740 are overplotted as observational constraints       {Miller2019_ApJL_J0030,Riley2019_ApJL_J0030, ...

$M$--$R$ curves for four externally validated EoSs with NN=valid and TOV=valid. Solid curves correspond to full TOV integrations, while the NICER credible regions for PSR~J0030 and PSR~J0740 are overplotted as observational constraints {Miller2019_ApJL_J0030,Riley2019_ApJL_J0030, ...

Empirical coverage for classification and regression under Standard and Mondrian     CP as a function of $ $. All curves track the nominal $1- $ within     sampling noise, indicating that the calibrated quantiles correctly characterize     the residual distribution. Mondrian's stratified calibrat...

Empirical coverage for classification and regression under Standard and Mondrian CP as a function of $ $. All curves track the nominal $1- $ within sampling noise, indicating that the calibrated quantiles correctly characterize the residual distribution. Mondrian's stratified calibrat...

–radius relations $M$--$R$ for the valid EoS subset (amber background), overlaid with NICER constraints for PSR~J0030+0451 and PSR~J0740+6620. Outer contour boundaries are solid; inner credible levels are dashed.

–radius relations $M$--$R$ for the valid EoS subset (amber background), overlaid with NICER constraints for PSR~J0030+0451 and PSR~J0740+6620. Outer contour boundaries are solid; inner credible levels are dashed.

Mean prediction–interval width for the four regression targets as a function of     $ $. Interval widths decrease monotonically as the acceptance threshold     relaxes. Mondrian yields narrower intervals when class–conditioned residuals     are less variable, reflecting improved efficiency withou...

Mean prediction–interval width for the four regression targets as a function of $ $. Interval widths decrease monotonically as the acceptance threshold relaxes. Mondrian yields narrower intervals when class–conditioned residuals are less variable, reflecting improved efficiency withou...

Certified Uncertainty for Surrogate Models of Neutron Star Equations of State via Mondrian Conformal Prediction. Marlon M. S. Mendes et. al. https://arxiv.org/abs/2602.19363

11.03.2026 00:35 👍 0 🔁 0 💬 0 📌 0
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Euclid preparation. Impact of galaxy intrinsic alignment modelling choices on Euclid 3x2pt cosmology. Euclid Collaboration: D. Navarro-Gironés (1 and 2 and 3) et. al. https://arxiv.org/abs/2602.16448

11.03.2026 00:34 👍 0 🔁 0 💬 0 📌 0
{Corner Plot of Fit Posteriors.

{Corner Plot of Fit Posteriors.

{Pre-fit Phase-folded Light Curve.

{Pre-fit Phase-folded Light Curve.

{Centroid Motion Analysis.

{Centroid Motion Analysis.

{Hot Jupiter Population Comparison.

{Hot Jupiter Population Comparison.

Statistical Validation and Photometric Characterization of the Hot Jupiter Candidate TOI 7475.01. Biel Escolà-Rodrigo https://arxiv.org/abs/2602.14840

11.03.2026 00:33 👍 1 🔁 0 💬 0 📌 0
Halo mass functions (HMFs) for CDM (solid lines) and ULDM (dashed lines, for $m_{22

Halo mass functions (HMFs) for CDM (solid lines) and ULDM (dashed lines, for $m_{22

The mass spectrum of SMBHs as a function of redshift.   The black horizontal line denotes the minimum masses of SMBH seeds  $M^{min

The mass spectrum of SMBHs as a function of redshift. The black horizontal line denotes the minimum masses of SMBH seeds $M^{min

The minimum mass $M_J$ (the thick lines) and the maximum mass $M_{upper

The minimum mass $M_J$ (the thick lines) and the maximum mass $M_{upper

Little Red Dots and Supermassive Black Hole Seed Formation in Ultralight Dark Matter Halos. Dongsu Bak et. al. https://arxiv.org/abs/2601.21676

11.03.2026 00:33 👍 1 🔁 0 💬 0 📌 0
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Euclid preparation. Galaxy power spectrum modelling in redshift space. Euclid Collaboration: B. Camacho Quevedo (1 and 2 and 3 and 4 and 5) et. al. https://arxiv.org/abs/2601.20826

11.03.2026 00:32 👍 0 🔁 0 💬 0 📌 0

Mathematical Anatomy of Neutrino Decoherence in Red Turbulence: A Fractional Calculus Approach. Yiwei Bao et. al. https://arxiv.org/abs/2601.20313

11.03.2026 00:31 👍 0 🔁 0 💬 0 📌 0
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SN 2024abvb: A Type Icn Supernova in the Outskirts of its Host Galaxy. Maokai Hu et. al. https://arxiv.org/abs/2601.01333

11.03.2026 00:30 👍 0 🔁 0 💬 0 📌 0
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Cosmic Himalayas in CROCODILE : Probing the Extreme Quasar Overdensities by Count-in-Cells analysis and Nearest Neighbor Distribution. Yuto Kuwayama et. al. https://arxiv.org/abs/2512.24966

11.03.2026 00:30 👍 0 🔁 0 💬 0 📌 0
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Discovering gravitational waveform distortions from lensing: a deep dive into GW231123. Juno C. L. Chan et. al. https://arxiv.org/abs/2512.16916

11.03.2026 00:29 👍 0 🔁 0 💬 0 📌 0
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The frame-dragging vector potential on galaxy scales from Dark-Matter-only Newtonian $N$-body simulations. William Beordo et. al. https://arxiv.org/abs/2512.08703

11.03.2026 00:28 👍 0 🔁 0 💬 0 📌 0
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Polarimetric and spectropolarimetric observations with FoReRo2: Instrument overview and standard star monitoring. Yanko Nikolov et. al. https://arxiv.org/abs/2512.05670

11.03.2026 00:28 👍 0 🔁 0 💬 0 📌 0