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arxiv: 2604.05428 · v1 · submitted 2026-04-07 · 🌌 astro-ph.HE · gr-qc

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Reconstruction of fast-rotating neutron star observables with the neural network

Lingxiao Wang, Wen Liu, Zhenyu Zhu

Authors on Pith no claims yet

Pith reviewed 2026-05-10 20:04 UTC · model grok-4.3

classification 🌌 astro-ph.HE gr-qc
keywords neutron starsequation of stateneural networksrotating neutron starsastrophysical inferencecausal networkscomputational astrophysicsrapid rotation
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The pith

Causal neural networks reconstruct fast-rotating neutron star observables thousands of times faster than traditional solvers.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

This paper develops causal convolutional neural networks to rapidly compute neutron star properties from an equation of state for static, Keplerian, and rotating cases. Traditional RNS calculations take around 30 minutes per configuration, which blocks statistical inference that needs thousands of evaluations. The networks are trained on RNS-generated data and validated on three equations of state, reproducing the original results to high accuracy. Evaluation time drops to about 50 milliseconds per case while the network architecture maintains the physical ordering of dependence on the equation of state. The speedup directly supports efficient inference analyses on the interiors of rapidly spinning neutron stars.

Core claim

The authors train causal convolutional neural networks on datasets produced by the RNS code to reconstruct neutron star observables. These networks preserve the chronological-like dependence of properties on the equation of state and deliver accurate results for static, Keplerian, and rotating configurations. Validation on the SFHo, SLy4, and DD2 equations of state confirms close agreement with direct RNS output. The trained models evaluate a full configuration for one equation of state in roughly 50 milliseconds, compared with typical RNS runtimes of 30 minutes, thereby enabling large-scale inference studies that involve rapidly rotating neutron stars.

What carries the argument

Causal convolutional neural networks that enforce chronological-like dependence of neutron star observables on the equation of state.

Load-bearing premise

Networks trained on a finite collection of equations of state and rotation rates will generalize accurately to arbitrary equations of state and rotation rates while preserving physical causal relations between inputs and outputs.

What would settle it

Compute network predictions for an equation of state withheld from training, at a high rotation rate near the mass-shedding limit, and compare the full set of output observables against independent RNS runs for the same central density and angular velocity.

Figures

Figures reproduced from arXiv: 2604.05428 by Lingxiao Wang, Wen Liu, Zhenyu Zhu.

Figure 1
Figure 1. Figure 1: The structure of causal convolutional networks for rotating configurations. For the other two networks (static and Keplerian), the structures are slightly different: they take only the one-array EoS input and use fewer (5) hidden layers and fewer (64) channels. Note that the different colored arrows in latent layes illustrate the causal receptive field of individual nodes at different sequence position. Pl… view at source ↗
Figure 2
Figure 2. Figure 2: The parity plots for the Keplerian-rotation network compare the ground truth and the predictions, shown on the horizontal and vertical axes, respectively. The data points in the training and test sets are denoted by blue and orange dots. The identity lines are shown as black dashed lines. The results for gravitational mass, equatorial radius and angular velocity are shown in the left, middle and right pane… view at source ↗
Figure 3
Figure 3. Figure 3: The same parity plots as in [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: The mass-radius relations of rotating NSs evaluated at the baseline axes ratios for SFHo (left), SLy4 (middle), and DD2 (right) EoS. The RNS ground truth and NN predictions are shown as lines and dots, respectively. Colors indicate different axes ratios, as well as the static and Kepler cases. been trained to sufficient accuracy to reconstruct the properties of rotating NSs. Therefore, we did not remove th… view at source ↗
Figure 5
Figure 5. Figure 5: The angular velocity as a function of mass for different EoS. The labels are the same as in the previous figures. baseline axes ratios. We then combine these results with the static and Kepler-rotating models and use interpolation to obtain the observables at intermediate rotation states (i.e., other values of rp/re). In [PITH_FULL_IMAGE:figures/full_fig_p007_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: The mass-radius relations for configurations with five values of Ω (0.2, 0.4, 0.6, 0.8, 1.0, in units of 104 s −1 ). The static and Kepler models are also included, and the labels for them, as well as for the RNS ground truth and the NN predictions, are the same as in previous figures. errors of NN prediction remain at a high level of precision. This conclusion also holds for the SLy4 EoS. Therefore, our i… view at source ↗
Figure 7
Figure 7. Figure 7: Other observables as a function of gravitational mass M or radius R for SFHo EoS. The labels are the same as in [PITH_FULL_IMAGE:figures/full_fig_p012_7.png] view at source ↗
read the original abstract

Rotation can significantly affect neutron-star (NS) properties, but accurate modeling of rapidly rotating NSs requires solving a two-dimensional, axially symmetric system, making traditional calculations too expensive for inference analyses that demand a large amount of model evaluations. We develop a causal convolutional neural networks that preserve the chronological-like dependence of NS properties on the equation of state (EoS) and rapidly reconstruct observables for static, Keplerian, and rotating configurations. Using \texttt{RNS}, we generate a dataset of NS observables and use it to train our networks. We validate our networks with three representative EoS (SFHo, SLy4, and DD2) and find that the they accurately reproduce the \texttt{RNS} results. The trained networks evaluate NS configurations for a single EoS in $\sim 50$ms, providing a substantial speedup over typical \texttt{RNS} runtimes of $\sim 30$ min and enabling efficient inference analyses involving rapidly rotating NSs.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 1 minor

Summary. The manuscript develops causal convolutional neural networks trained on RNS-generated datasets to reconstruct neutron-star observables (including for static, Keplerian, and rotating configurations) directly from the equation of state. It reports that the networks reproduce RNS results for the three EoS SFHo, SLy4, and DD2, with per-EoS evaluation times of ~50 ms versus ~30 min for direct RNS integration, thereby enabling efficient inference analyses involving rapidly rotating neutron stars.

Significance. If the reported accuracy and generalization hold, the work would supply a practical surrogate model that removes the computational bottleneck of 2D rotating-NS structure calculations, allowing Bayesian inference or population studies that require thousands of model evaluations to become feasible within current resources.

major comments (2)
  1. [Abstract / Results] Abstract and Results section: the claim that the networks 'accurately reproduce the RNS results' on SFHo, SLy4, and DD2 is unsupported by any quantitative error metrics (maximum or median relative errors on equatorial radius, moment of inertia, or Kepler frequency), training-set size, or explicit statement of whether these three EoS were held out from training.
  2. [Methods / Validation] Methods and Validation sections: no information is given on the diversity or number of EoS used to generate the training set, the distribution of rotation rates (especially near the Kepler limit), or any test of generalization to EoS stiffness or spin values outside the three validation cases; without these the central claim that the networks enable inference for arbitrary EoS remains unproven.
minor comments (1)
  1. [Abstract] Abstract contains a typographical error: 'the they accurately' should read 'they accurately'.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments, which identify important omissions that will improve the manuscript. We address each point below and will revise the paper to incorporate the requested quantitative details and dataset information.

read point-by-point responses
  1. Referee: [Abstract / Results] Abstract and Results section: the claim that the networks 'accurately reproduce the RNS results' on SFHo, SLy4, and DD2 is unsupported by any quantitative error metrics (maximum or median relative errors on equatorial radius, moment of inertia, or Kepler frequency), training-set size, or explicit statement of whether these three EoS were held out from training.

    Authors: We agree that quantitative error metrics are needed to support the accuracy statement. In the revised manuscript we will add explicit values for the maximum and median relative errors on equatorial radius, moment of inertia, and Kepler frequency for SFHo, SLy4, and DD2. We will also report the training-set size and state that these three EoS were excluded from training and used exclusively for validation. revision: yes

  2. Referee: [Methods / Validation] Methods and Validation sections: no information is given on the diversity or number of EoS used to generate the training set, the distribution of rotation rates (especially near the Kepler limit), or any test of generalization to EoS stiffness or spin values outside the three validation cases; without these the central claim that the networks enable inference for arbitrary EoS remains unproven.

    Authors: We acknowledge that the current text lacks sufficient detail on the training data and generalization tests. The training set was generated from a broad collection of EoS spanning a range of stiffnesses, with rotation rates sampled up to the Kepler limit. In the revision we will specify the number of EoS employed, describe the rotation-rate distribution, and present additional validation results on EoS stiffnesses and spin values outside the three reported cases. These additions will directly support the applicability to arbitrary EoS in inference studies. revision: yes

Circularity Check

0 steps flagged

No circularity: standard supervised surrogate on external RNS simulator

full rationale

The paper generates training data with the independent RNS code, trains a causal CNN to map EoS inputs to NS observables, and validates reproduction on three EoS. This is ordinary supervised regression with no derivation, ansatz, or prediction that reduces to its own fitted inputs by construction. No self-citations are load-bearing for the central claim, and the speedup follows directly from NN inference speed versus RNS runtime. The result is self-contained against the external benchmark.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

The central claim rests on the empirical performance of a neural network trained to emulate RNS output; no new physical axioms or invented entities are introduced beyond the standard assumptions already present in the RNS code and the chosen equations of state.

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90 extracted references · 90 canonical work pages · 1 internal anchor

  1. [1]

    2017, PhRvL, 119, 161101, doi: 10.1103/PhysRevLett.119.161101

    Abbott, B. P., Abbott, R., Abbott, T. D., et al. 2017, Phys. Rev. Lett., 119, 161101, doi: 10.1103/PhysRevLett.119.161101 —. 2018, Physical Review Letters, 121, 161101, doi: 10.1103/PhysRevLett.121.161101 —. 2019, Physical Review X, 9, 011001, doi: 10.1103/PhysRevX.9.011001 —. 2020, ApJL, 892, L3, doi: 10.3847/2041-8213/ab75f5

  2. [2]

    2022, ApJL, 939, L34, doi: 10.3847/2041-8213/ac9b2a

    Altiparmak, S., Ecker, C., & Rezzolla, L. 2022, ApJL, 939, L34, doi: 10.3847/2041-8213/ac9b2a

  3. [3]

    Andersson, N., & Comer, G. L. 2001, Classical and Quantum Gravity, 18, 969, doi: 10.1088/0264-9381/18/6/302

  4. [4]

    Gravitational-wave constraints on the neutron-star- matter Equation of State.Phys

    Annala, E., Gorda, T., Kurkela, A., & Vuorinen, A. 2018, PhRvL, 120, 172703, doi: 10.1103/PhysRevLett.120.172703

  5. [5]

    G., Pleunis, Z., Hessels, J

    Bassa, C. G., Pleunis, Z., Hessels, J. W. T., et al. 2017, ApJL, 846, L20, doi: 10.3847/2041-8213/aa8400

  6. [6]

    1971, ApJ, 170, 299, doi: 10.1086/151216

    Baym, G., Pethick, C., & Sutherland, P. 1971, ApJ, 170, 299, doi: 10.1086/151216

  7. [7]

    1998, PhRvD, 58, 104020, doi: 10.1103/PhysRevD.58.104020

    Bonazzola, S., Gourgoulhon, E., & Marck, J.-A. 1998, PhRvD, 58, 104020, doi: 10.1103/PhysRevD.58.104020

  8. [8]

    2021, MNRAS, 505, 1661, doi: 10.1093/mnras/stab1287

    Breschi, M., Perego, A., Bernuzzi, S., et al. 2021, MNRAS, 505, 1661, doi: 10.1093/mnras/stab1287

  9. [9]

    1998, NuPhA, 635, 231, doi: 10.1016/S0375-9474(98)00180-8

    Schaeffer, R. 1998, NuPhA, 635, 231, doi: 10.1016/S0375-9474(98)00180-8

  10. [10]

    2024, ApJL, 971, L20, doi: 10.3847/2041-8213/ad5a6f

    Choudhury, D., Salmi, T., Vinciguerra, S., et al. 2024, ApJL, 971, L20, doi: 10.3847/2041-8213/ad5a6f

  11. [11]

    B., Shapiro, S

    Cook, G. B., Shapiro, S. L., & Teukolsky, S. A. 1994, ApJ, 422, 227, doi: 10.1086/173721

  12. [12]

    W., Dietrich, T., Margalit, B., & Metzger, B

    Coughlin, M. W., Dietrich, T., Margalit, B., & Metzger, B. D. 2019, MNRAS, 489, L91, doi: 10.1093/mnrasl/slz133

  13. [13]

    Physical Review D , author =

    Dietrich, T., Samajdar, A., Khan, S., et al. 2019, PhRvD, 100, 044003, doi: 10.1103/PhysRevD.100.044003

  14. [14]

    2025, PhRvD, 112, 103023, doi: 10.1103/krc7-kz2l Flanagan, ´E

    Finch, E., Legred, I., Chatziioannou, K., et al. 2025, PhRvD, 112, 103023, doi: 10.1103/krc7-kz2l Flanagan, ´E. ´E., & Hinderer, T. 2008, PhRvD, 77, 021502, doi: 10.1103/PhysRevD.77.021502

  15. [15]

    T., Pennucci, T

    Fonseca, E., Cromartie, H. T., Pennucci, T. T., et al. 2021, ApJL, 915, L12, doi: 10.3847/2041-8213/ac03b8

  16. [16]

    2018, PhRvD, 98, 023019, doi: 10.1103/PhysRevD.98.023019 —

    Fujimoto, Y., Fukushima, K., & Murase, K. 2018, PhRvD, 98, 023019, doi: 10.1103/PhysRevD.98.023019 —. 2020, PhRvD, 101, 054016, doi: 10.1103/PhysRevD.101.054016

  17. [17]

    2022, PhRvD, 106, 123529, doi: 10.1103/PhysRevD.106.123529

    Ghosh, T., Biswas, B., & Bose, S. 2022, PhRvD, 106, 123529, doi: 10.1103/PhysRevD.106.123529

  18. [18]

    1999, A&A, 349, 851, doi: 10.48550/arXiv.astro-ph/9907225

    Gourgoulhon, E., Haensel, P., Livine, R., et al. 1999, A&A, 349, 851, doi: 10.48550/arXiv.astro-ph/9907225

  19. [19]

    K., Puecher, A., Pang, P

    Gupta, P. K., Puecher, A., Pang, P. T. H., et al. 2022, arXiv e-prints, arXiv:2205.01182, doi: 10.48550/arXiv.2205.01182

  20. [20]

    2023a, Science Bulletin, 68, 913, doi: 10.1016/j.scib.2023.04.007

    Han, M.-Z., Huang, Y.-J., Tang, S.-P., & Fan, Y.-Z. 2023a, Science Bulletin, 68, 913, doi: 10.1016/j.scib.2023.04.007

  21. [21]

    2021, ApJ, 919, 11, doi: 10.3847/1538-4357/ac11f8

    Han, M.-Z., Jiang, J.-L., Tang, S.-P., & Fan, Y.-Z. 2021, ApJ, 919, 11, doi: 10.3847/1538-4357/ac11f8

  22. [22]

    2023b, ApJ, 950, 77, doi: 10.3847/1538-4357/acd050

    Han, M.-Z., Tang, S.-P., & Fan, Y.-Z. 2023b, ApJ, 950, 77, doi: 10.3847/1538-4357/acd050

  23. [23]

    Hessels, J. W. T., Ransom, S. M., Stairs, I. H., et al. 2006, Science, 311, 1901, doi: 10.1126/science.1123430

  24. [24]
  25. [25]

    D., Lang, R

    Hinderer, T., Lackey, B. D., Lang, R. N., & Read, J. S. 2010, PhRvD, 81, 123016, doi: 10.1103/PhysRevD.81.123016

  26. [26]

    2022, ApJ, 926, 196, doi: 10.3847/1538-4357/ac490e

    Belczynski, K. 2022, ApJ, 926, 196, doi: 10.3847/1538-4357/ac490e

  27. [27]

    J., & Kehl, M

    Hu, H., Kramer, M., Wex, N., Champion, D. J., & Kehl, M. S. 2020, MNRAS, 497, 3118, doi: 10.1093/mnras/staa2107

  28. [28]

    2024, PhRvD, 109, 103035, doi: 10.1103/PhysRevD.109.103035

    Huxford, R., Kashyap, R., Borhanian, S., et al. 2024, PhRvD, 109, 103035, doi: 10.1103/PhysRevD.109.103035

  29. [29]

    Astrophys J 941(2):208

    Iacovelli, F., Mancarella, M., Foffa, S., & Maggiore, M. 2022, ApJ, 941, 208, doi: 10.3847/1538-4357/ac9cd4

  30. [30]

    Phys Rev D 108(12):122006

    Iacovelli, F., Mancarella, M., Mondal, C., et al. 2023, PhRvD, 108, 122006, doi: 10.1103/PhysRevD.108.122006

  31. [31]

    1989, MNRAS, 237, 355, doi: 10.1093/mnras/237.2.355

    Komatsu, H., Eriguchi, Y., & Hachisu, I. 1989, MNRAS, 237, 355, doi: 10.1093/mnras/237.2.355

  32. [32]

    H., Manchester, R

    Kramer, M., Stairs, I. H., Manchester, R. N., et al. 2021, Physical Review X, 11, 041050, doi: 10.1103/PhysRevX.11.041050

  33. [33]

    2025, PhRvD, 112, 063003, doi: 10.1103/9kh9-xfpd

    Chatziioannou, K. 2025, PhRvD, 112, 063003, doi: 10.1103/9kh9-xfpd

  34. [34]

    O., Chatziioannou, K., & Essick, R

    Legred, I., Sy-Garcia, B. O., Chatziioannou, K., & Essick, R. 2024, PhRvD, 109, 023020, doi: 10.1103/PhysRevD.109.023020

  35. [35]

    2016, PhRvD, 94, 083010, doi: 10.1103/PhysRevD.94.083010

    Li, A., Zhang, B., Zhang, N.-B., et al. 2016, PhRvD, 94, 083010, doi: 10.1103/PhysRevD.94.083010

  36. [36]

    2017, ApJ, 844, 41, doi: 10.3847/1538-4357/aa7a00

    Li, A., Zhu, Z.-Y., & Zhou, X. 2017, ApJ, 844, 41, doi: 10.3847/1538-4357/aa7a00

  37. [37]

    2024, PhRvD, 110, 103040, doi: 10.1103/PhysRevD.110.103040

    Li, B.-A., Grundler, X., Xie, W.-J., & Zhang, N.-B. 2024, PhRvD, 110, 103040, doi: 10.1103/PhysRevD.110.103040

  38. [38]

    2025, PhRvD, 111, 074026, doi: 10.1103/PhysRevD.111.074026 10

    Li, R., Han, S., Lin, Z., et al. 2025, PhRvD, 111, 074026, doi: 10.1103/PhysRevD.111.074026 10

  39. [39]

    2010, PhRvD, 82, 103011, doi: 10.1103/PhysRevD.82.103011 —

    Lindblom, L. 2010, PhRvD, 82, 103011, doi: 10.1103/PhysRevD.82.103011 —. 2022, PhRvD, 105, 063031, doi: 10.1103/PhysRevD.105.063031

  40. [40]

    2024, PhRvD, 110, 083030, doi: 10.1103/PhysRevD.110.083030

    Lindblom, L., & Zhou, T. 2024, PhRvD, 110, 083030, doi: 10.1103/PhysRevD.110.083030

  41. [41]

    Science Case for the Einstein Telescope

    Maggiore, M., Van Den Broeck, C., Bartolo, N., et al. 2020, JCAP, 2020, 050, doi: 10.1088/1475-7516/2020/03/050

  42. [42]

    Margalit, B., & Metzger, B. D. 2017, ApJL, 850, L19, doi: 10.3847/2041-8213/aa991c

  43. [43]

    2025, arXiv e-prints, arXiv:2508.08750, doi: 10.48550/arXiv.2508.08750

    Markin, I., Puecher, A., Bulla, M., & Dietrich, T. 2025, arXiv e-prints, arXiv:2508.08750, doi: 10.48550/arXiv.2508.08750

  44. [44]

    C., Lamb, F

    Miller, M. C., Lamb, F. K., Dittmann, A. J., et al. 2019, Astrophys. J. Lett., 887, L24, doi: 10.3847/2041-8213/ab50c5 —. 2021, Astrophys. J. Lett., 918, L28, doi: 10.3847/2041-8213/ac089b

  45. [45]

    2020, A&A, 642, A78, doi: 10.1051/0004-6361/202038130

    Morawski, F., & Bejger, M. 2020, A&A, 642, A78, doi: 10.1051/0004-6361/202038130

  46. [46]

    R., Weih, L

    Most, E. R., Weih, L. R., Rezzolla, L., & Schaffner-Bielich, J. 2018, PhRvL, 120, 261103, doi: 10.1103/PhysRevLett.120.261103

  47. [47]

    2024, ApJ, 962, 61, doi: 10.3847/1538-4357/ad1758

    Musolino, C., Ecker, C., & Rezzolla, L. 2024, ApJ, 962, 61, doi: 10.3847/1538-4357/ad1758

  48. [48]

    R., & Rezzolla, L

    Nathanail, A., Most, E. R., & Rezzolla, L. 2021, ApJL, 908, L28, doi: 10.3847/2041-8213/abdfc6

  49. [49]

    2025, Classical and Quantum Gravity, 42, 205008, doi: 10.1088/1361-6382/ae1094

    Ng, S., Legred, I., Suleiman, L., et al. 2025, Classical and Quantum Gravity, 42, 205008, doi: 10.1088/1361-6382/ae1094

  50. [50]

    1998, A&AS, 132, 431, doi: 10.1051/aas:1998304

    Nozawa, T., Stergioulas, N., Gourgoulhon, E., & Eriguchi, Y. 1998, A&AS, 132, 431, doi: 10.1051/aas:1998304

  51. [51]

    J., Tootle, S

    Papenfort, L. J., Tootle, S. D., Grandcl´ ement, P., Most, E. R., & Rezzolla, L. 2021, PhRvD, 104, 024057, doi: 10.1103/PhysRevD.104.024057

  52. [52]

    The third generation of gravitational wave observatories and their science reach

    Punturo, M., Abernathy, M., Acernese, F., et al. 2010, Classical and Quantum Gravity, 27, 084007, doi: 10.1088/0264-9381/27/8/084007

  53. [53]

    2018, ApJL, 852, L29, doi: 10.3847/2041-8213/aaa402

    Radice, D., Perego, A., Zappa, F., & Bernuzzi, S. 2018, ApJL, 852, L29, doi: 10.3847/2041-8213/aaa402

  54. [54]

    A., ¨Ozel, F., & Psaltis, D

    Raithel, C. A., ¨Ozel, F., & Psaltis, D. 2018, ApJL, 857, L23, doi: 10.3847/2041-8213/aabcbf

  55. [55]

    T., Somasundaram, R., De, S., et al

    Reed, B. T., Somasundaram, R., De, S., et al. 2024, ApJ, 974, 285, doi: 10.3847/1538-4357/ad737c

  56. [56]

    Cosmic Explorer: The U.S. Contribution to Gravitational-Wave Astronomy beyond LIGO

    Reitze, D., Adhikari, R. X., Ballmer, S., et al. 2019, in Bulletin of the American Astronomical Society, Vol. 51, 35, doi: 10.48550/arXiv.1907.04833

  57. [57]

    E., Watts, A

    Riley, T. E., Watts, A. L., Bogdanov, S., et al. 2019, Astrophys. J. Lett., 887, L21, doi: 10.3847/2041-8213/ab481c

  58. [58]

    E., Watts, A

    Riley, T. E., Watts, A. L., Ray, P. S., et al. 2021, Astrophys. J. Lett., 918, L27, doi: 10.3847/2041-8213/ac0a81

  59. [59]

    , keywords =

    Romani, R. W., Kandel, D., Filippenko, A. V., Brink, T. G., & Zheng, W. 2022, ApJL, 934, L17, doi: 10.3847/2041-8213/ac8007

  60. [60]

    2012, Classical and Quantum Gravity, 29, 124013, doi: 10.1088/0264-9381/29/12/124013

    Sathyaprakash, B., Abernathy, M., Acernese, F., et al. 2012, Classical and Quantum Gravity, 29, 124013, doi: 10.1088/0264-9381/29/12/124013

  61. [61]

    Shawqi, S., Konstantinou, A., & Morsink, S. M. 2025, arXiv e-prints, arXiv:2508.18434, doi: 10.48550/arXiv.2508.18434

  62. [62]

    2022, JCAP, 2022, 071, doi: 10.1088/1475-7516/2022/08/071 —

    Soma, S., Wang, L., Shi, S., St ¨ocker, H., & Zhou, K. 2022, JCAP, 2022, 071, doi: 10.1088/1475-7516/2022/08/071 —. 2023, PhRvD, 107, 083028, doi: 10.1103/PhysRevD.107.083028

  63. [63]

    W., Hempel , M., & Fischer , T

    Steiner, A. W., Hempel, M., & Fischer, T. 2013, ApJ, 774, 17, doi: 10.1088/0004-637X/774/1/17

  64. [64]

    Stergioulas, N., & Friedman, J. L. 1995, ApJ, 444, 306, doi: 10.1086/175605

  65. [65]

    F., Gulminelli, F., & Read, J

    Suleiman, L., Fantina, A. F., Gulminelli, F., & Read, J. 2025, arXiv e-prints, arXiv:2512.05315, doi: 10.48550/arXiv.2512.05315

  66. [66]

    D., Jacques, T

    Tootle, S. D., Jacques, T. P., & Cassing, M. 2026, arXiv e-prints, arXiv:2601.05176, doi: 10.48550/arXiv.2601.05176

  67. [67]

    2020, ApJ, 897, 165, doi: 10.3847/1538-4357/ab99c1

    Traversi, S., Char, P., & Pagliara, G. 2020, ApJ, 897, 165, doi: 10.3847/1538-4357/ab99c1

  68. [68]

    2025, PhRvD, 112, 043018, doi: 10.1103/bmb3-ktz6

    Tu, Z., Sun, X., Han, S., Miao, Z., & Li, A. 2025, PhRvD, 112, 043018, doi: 10.1103/bmb3-ktz6

  69. [69]

    Typel, S., R¨opke, G., Kl¨ahn, T., Blaschke, D., & Wolter, H. H. 2010, PhRvC, 81, 015803, doi: 10.1103/PhysRevC.81.015803

  70. [70]

    C., & Stuchl´ ık, Z

    Urbanec, M., Miller, J. C., & Stuchl´ ık, Z. 2013, MNRAS, 433, 1903, doi: 10.1093/mnras/stt858 van den Oord, A., Dieleman, S., Zen, H., et al. 2016, arXiv e-prints, arXiv:1609.03499, doi: 10.48550/arXiv.1609.03499

  71. [71]

    2024, arXiv e-prints, arXiv:2407.15753, doi: 10.48550/arXiv.2407.15753

    Vilkha, A., Yelikar, A., O’Shaughnessy, R., & Read, J. 2024, arXiv e-prints, arXiv:2407.15753, doi: 10.48550/arXiv.2407.15753

  72. [72]

    Walker, K., Smith, R., Thrane, E., & Reardon, D. J. 2024, PhRvD, 110, 043013, doi: 10.1103/PhysRevD.110.043013

  73. [73]

    2020, ApJS, 250, 6, doi: 10.3847/1538-4365/aba2f3

    Wang, B., Zhu, Z., Li, A., & Zhao, W. 2020, ApJS, 250, 6, doi: 10.3847/1538-4365/aba2f3

  74. [74]

    2018, PhRvC, 98, 054618, doi: 10.1103/PhysRevC.98.054618

    Wang, R., Chen, L.-W., & Zhou, Y. 2018, PhRvC, 98, 054618, doi: 10.1103/PhysRevC.98.054618

  75. [75]

    2025, PhRvC, 111, 054605, doi: 10.1103/PhysRevC.111.054605 11

    Wang, S.-P., Li, X., Wang, R., Ye, J.-T., & Chen, L.-W. 2025, PhRvC, 111, 054605, doi: 10.1103/PhysRevC.111.054605 11

  76. [76]

    2024, PhRvC, 109, 054623, doi: 10.1103/PhysRevC.109.054623

    Wang, S.-P., Wang, R., Ye, J.-T., & Chen, L.-W. 2024, PhRvC, 109, 054623, doi: 10.1103/PhysRevC.109.054623

  77. [77]

    R., Most, E

    Weih, L. R., Most, E. R., & Rezzolla, L. 2019, ApJ, 881, 73, doi: 10.3847/1538-4357/ab2edd

  78. [78]

    Wouters, T., Pang, P. T. H., Koehn, H., et al. 2025a, arXiv e-prints, arXiv:2504.15893, doi: 10.48550/arXiv.2504.15893 —. 2025b, PhRvD, 112, 043037, doi: 10.1103/v2y8-kxvx

  79. [79]

    2025, arXiv e-prints, arXiv:2502.09200, doi: 10.48550/arXiv.2502.09200

    Wu, Z., Biswas, B., & Rosswog, S. 2025, arXiv e-prints, arXiv:2502.09200, doi: 10.48550/arXiv.2502.09200

  80. [80]

    B., O’Shaughnessy, R., Wysocki, D., & Wade, L

    Yelikar, A. B., O’Shaughnessy, R., Wysocki, D., & Wade, L. 2024, arXiv e-prints, arXiv:2410.14674, doi: 10.48550/arXiv.2410.14674

Showing first 80 references.