Recognition: unknown
Parameter Estimation Horizon of Core-Collapse Supernovae with Current and Next-Generation Gravitational-Wave Detectors
Pith reviewed 2026-05-08 15:55 UTC · model grok-4.3
The pith
Machine learning on gravitational-wave signals from core-collapse supernovae can constrain core rotation out to more than 100 kpc with next-generation detectors for favorable orientations.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Parameter estimation of peak frequency, peak amplitude, and core rotation from the bounce and early ring-down gravitational-wave signal of rotating core-collapse supernovae is robust to bounce-time uncertainty in the Fourier domain but degrades for near face-on inclinations; for optimal orientations, next-generation detector sensitivities extend the distance horizon for rotation constraints beyond 100 kpc.
What carries the argument
Machine learning regression applied to Fourier-domain gravitational-wave signals to infer peak frequency, peak amplitude, and progenitor core rotation.
If this is right
- Bounce-time uncertainty has negligible impact on parameter recovery when the analysis uses the Fourier domain.
- Inclinations that place the rotation axis near the line of sight cause substantial loss of accuracy in all recovered parameters.
- Next-generation detectors extend the rotation-constraint horizon beyond 100 kpc for optimally oriented sources.
- The method remains applicable across a range of progenitor masses and nuclear equations of state.
Where Pith is reading between the lines
- Combined gravitational-wave and neutrino observations of the same event could cross-check the rotation values extracted by the machine-learning pipeline.
- Applying the trained models to archival data from current detectors could set preliminary upper limits on core rotation for nearby supernovae even without a positive detection.
- Extending the training set to include more varied explosion dynamics would test whether the current distance horizon holds for a broader class of signals.
Load-bearing premise
Machine learning models trained on a finite collection of simulated signals from chosen progenitors and equations of state will produce unbiased estimates when applied to real gravitational-wave data.
What would settle it
Detection of a core-collapse supernova gravitational-wave signal with independently known orientation and rotation, followed by comparison of the machine-learning rotation estimate against that independent value.
Figures
read the original abstract
Core-collapse supernovae (CCSNe) are powerful sources of gravitational waves (GWs). These signals propagate essentially unobstructed, providing a unique probe of the supernova central engine. In this work, we investigate parameter estimation from the bounce and early ring-down GW signal of rotating CCSNe using machine learning. We infer the peak frequency and peak amplitude of the signal as well as the rotation of the core. We extend previous studies in several directions. We consider a range of progenitor models and nuclear equations of state, and we assess the impact of key physical uncertainties, including bounce-time uncertainty and source inclination. We incorporate both current detector noise and the projected sensitivities of next-generation observatories. We find that uncertainty in the bounce time does not significantly affect parameter estimation when the analysis is performed in the Fourier domain. In contrast, orientations when the rotation axis is near the line of sight substantially degrade performance. For optimal orientations, next-generation detectors can constrain rotation out to distances exceeding 100 kpc.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript develops a machine-learning framework to infer the peak frequency, peak amplitude, and core rotation rate from the bounce and early ring-down gravitational-wave signals of rotating core-collapse supernovae. It employs a suite of 2D/3D numerical simulations spanning multiple progenitors and equations of state, tests robustness to bounce-time uncertainty in the Fourier domain, examines orientation dependence, and folds in noise curves for both current and next-generation detectors. The principal results are that Fourier-domain analysis is insensitive to bounce-time jitter, near face-on orientations substantially degrade performance, and next-generation detectors can constrain rotation beyond 100 kpc for optimal orientations.
Significance. If the reported ML performance generalizes, the work would meaningfully extend the science reach of gravitational-wave observations of core-collapse supernovae by showing that rotation can be constrained at extragalactic distances with future detectors, thereby offering a new observable for the supernova central engine.
major comments (2)
- [Abstract] Abstract and results on the 100 kpc horizon: the headline claim that next-generation detectors constrain rotation beyond 100 kpc for optimal orientations is obtained by feeding simulated peak-frequency and peak-amplitude values into ML regressors trained on a finite progenitor/EOS suite. No quantitative assessment is provided of systematic offsets that would arise if real signals include unmodeled 3D convective overturn, magnetic amplification, or neutrino-transport shifts in bounce frequency (tens of Hz), which directly affect the two summary statistics used by the regressors at low SNR.
- The Fourier-domain robustness test addresses only bounce-time jitter; it does not test robustness to morphology mismatch between the training ensemble and nature (e.g., full 3D turbulence altering the ring-down spectrum). Because the ML mapping is learned from the training distribution, any such mismatch would propagate directly into biased rotation posteriors at the distances claimed.
minor comments (2)
- Clarify the exact architecture, hyper-parameter choices, and cross-validation procedure used for the ML regressors; these details are essential for reproducibility and for judging generalization.
- The orientation-dependence results would benefit from an explicit table or figure showing the degradation in rotation uncertainty as a function of inclination angle for each detector class.
Simulated Author's Rebuttal
We thank the referee for their careful reading and constructive feedback. We address the major comments point by point below, agreeing that additional discussion of limitations is needed. We will revise the manuscript to incorporate these points.
read point-by-point responses
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Referee: [Abstract] Abstract and results on the 100 kpc horizon: the headline claim that next-generation detectors constrain rotation beyond 100 kpc for optimal orientations is obtained by feeding simulated peak-frequency and peak-amplitude values into ML regressors trained on a finite progenitor/EOS suite. No quantitative assessment is provided of systematic offsets that would arise if real signals include unmodeled 3D convective overturn, magnetic amplification, or neutrino-transport shifts in bounce frequency (tens of Hz), which directly affect the two summary statistics used by the regressors at low SNR.
Authors: We agree that our training ensemble is finite and does not capture all possible physical effects. While the suite spans multiple progenitors and equations of state, we have not performed a quantitative assessment of systematic shifts from full 3D convection, magnetic amplification, or neutrino-transport details. In the revised manuscript we will add a dedicated limitations section that discusses these potential biases, their likely impact on the summary statistics at low SNR, and the resulting uncertainty in the reported horizons. We will also moderate the abstract language to reflect these caveats. revision: yes
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Referee: The Fourier-domain robustness test addresses only bounce-time jitter; it does not test robustness to morphology mismatch between the training ensemble and nature (e.g., full 3D turbulence altering the ring-down spectrum). Because the ML mapping is learned from the training distribution, any such mismatch would propagate directly into biased rotation posteriors at the distances claimed.
Authors: The referee is correct that the existing test is limited to bounce-time jitter and does not address broader morphological differences that could arise from three-dimensional turbulence or other unmodeled physics. Because the regressors are trained on the specific distribution of our simulations, such mismatches could introduce biases. We will revise the manuscript to include an explicit statement of this limitation in the discussion, clarifying that the quoted performance assumes signals drawn from the training distribution. Expanded simulation libraries will be required for a more complete robustness test. revision: partial
Circularity Check
No significant circularity: ML inference trained on external simulations and evaluated on held-out cases
full rationale
The derivation chain trains ML regressors on a finite suite of numerical CCSN simulations (varying progenitors, EOS, rotation) to map Fourier-domain peak frequency and amplitude to core rotation rate. Performance metrics and distance horizons (>100 kpc for optimal orientations with next-gen detectors) are obtained by applying the trained models to separate test waveforms injected at varying distances and orientations. No equation or claim reduces by construction to a fitted parameter from the same data; bounce-time robustness is tested via explicit Fourier-domain shifts rather than assumed. External simulation inputs and cross-validation prevent self-definitional or fitted-input-called-prediction circularity. Minor self-citations to prior simulation suites are not load-bearing for the central claims.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Gravitational-wave signals from rotating CCSNe exhibit identifiable peak frequency and amplitude features in the Fourier domain that correlate with core rotation.
- domain assumption Numerical simulations with the selected progenitors and nuclear equations of state adequately sample the relevant signal variations.
Reference graph
Works this paper leans on
-
[1]
The LIGO Scientific Collaboration, the Virgo Col- laboration, the KAGRA Collaboration, A. G. Abac, 10 I. Abouelfettouh, F. Acernese, and K. e. a. Ackley, GWTC-4.0: Updating the Gravitational-Wave Tran- sient Catalog with Observations from the First Part of the Fourth LIGO-Virgo-KAGRA Observing Run, arXiv e-prints , arXiv:2508.18082 (2025), arXiv:2508.1808...
work page internal anchor Pith review arXiv 2025
-
[2]
A. Mezzacappa and M. Zanolin, Gravitational Waves from Neutrino-Driven Core Collapse Supernovae: Pre- dictions, Detection, and Parameter Estimation, arXiv e-prints , arXiv:2401.11635 (2024), arXiv:2401.11635 [astro-ph.HE]
-
[3]
D. Vartanyan, A. Burrows, T. Wang, M. S. B. Coleman, and C. J. White, Gravitational-wave signature of core- collapse supernovae, Phys. Rev. D 107, 103015 (2023), arXiv:2302.07092 [astro-ph.HE]
- [4]
-
[5]
B. P. Abbott, R. Abbott, T. D. Abbott, S. Abraham, and F. Acernese (LIGO Scientific Collaboration and Virgo Collaboration and ASAS-SN Collaboration and DLT40 Collaboration), Optically targeted search for gravitational waves emitted by core-collapse supernovae during the first and second observing runs of advanced ligo and advanced virgo, Phys. Rev. D 101,...
2020
-
[6]
M. J. Szczepa´ nczyk, Y. Zheng, J. M. Antelis, M. Ben- jamin, M.-A. Bizouard, A. Casallas-Lagos, P. Cerd´ a- Dur´ an, D. Davis, D. Gondek-Rosi´ nska, S. Klimenko, C. Moreno, M. Obergaulinger, J. Powell, D. Ramirez, B. Ratto, C. Richardson, A. Rijal, A. L. Stuver, P. Szewczyk, G. Vedovato, M. Zanolin, I. Bartos, S. Bhaumik, T. Bulik, M. Drago, J. A. Font, ...
2024
-
[7]
V. Srivastava, S. Ballmer, D. A. Brown, C. Afle, A. Bur- rows, D. Radice, and D. Vartanyan, Detection prospects of core-collapse supernovae with supernova-optimized third-generation gravitational-wave detectors, Phys. Rev. D 100, 043026 (2019), arXiv:1906.00084 [gr-qc]
- [8]
-
[9]
T. Ertl, H.-T. Janka, S. E. Woosley, T. Sukhbold, and M. Ugliano, A Two-parameter Criterion for Classify- ing the Explodability of Massive Stars by the Neutrino- driven Mechanism, Astrophys. J. 818, 124 (2016), arXiv:1503.07522 [astro-ph.SR]
-
[10]
L. Boccioli, D. Vartanyan, E. P. O’Connor, and D. Kasen, Neutrino heating in 1D, 2D, and 3D core- collapse supernovae: characterizing the explosion of high-compactness stars, MNRAS 540, 3885 (2025), arXiv:2501.06784 [astro-ph.HE]
-
[11]
H.-T. Janka, Conditions for shock revival by neutrino heating in core-collapse supernovae, A&A 368, 527 (2001), arXiv:astro-ph/0008432 [astro-ph]
-
[12]
A. Burrows, L. Dessart, E. Livne, C. D. Ott, and J. Murphy, Simulations of Magnetically Driven Super- nova and Hypernova Explosions in the Context of Rapid Rotation, Astrophys. J. 664, 416 (2007), arXiv:astro- ph/0702539
-
[13]
A. Burrows, Colloquium: Perspectives on core-collapse supernova theory, Reviews of Modern Physics 85, 245 (2013), arXiv:1210.4921 [astro-ph.SR]
-
[14]
E. O’Connor and C. D. Ott, Black Hole Formation in Failing Core-Collapse Supernovae, Astrophys. J. 730, 70 (2011), arXiv:1010.5550 [astro-ph.HE]
-
[15]
K. Nakamura, S. Horiuchi, M. Tanaka, K. Hayama, T. Takiwaki, and K. Kotake, Multimessenger signals of long-term core-collapse supernova simulations: syn- ergetic observation strategies, Mon. Not. Roy. Astron. Soc. 461, 3296 (2016), arXiv:1602.03028 [astro-ph.HE]
- [16]
-
[17]
B. M¨ uller, H.-T. Janka, and A. Marek, A New Multi- dimensional General Relativistic Neutrino Hydrody- namics Code of Core-collapse Supernovae. III. Gravita- tional Wave Signals from Supernova Explosion Models, Astrophys. J. 766, 43 (2013), arXiv:1210.6984 [astro- ph.SR]
-
[18]
V. Morozova, D. Radice, A. Burrows, and D. Var- tanyan, The Gravitational Wave Signal from Core- collapse Supernovae, Astrophys. J. 861, 10 (2018), arXiv:1801.01914 [astro-ph.HE]
-
[19]
A. Torres-Forn´ e, P. Cerd´ a-Dur´ an, M. Obergaulinger, B. M¨ uller, and J. A. Font, Universal Relations for Gravitational-Wave Asteroseismology of Protoneu- tron Stars, Phys. Rev. Lett. 123, 051102 (2019), arXiv:1902.10048 [gr-qc]
-
[20]
J. Powell and B. M¨ uller, Inferring astrophysical parame- ters of core-collapse supernovae from their gravitational- wave emission, Phys. Rev. D 105, 063018 (2022), arXiv:2201.01397 [astro-ph.HE]
-
[21]
Burrows and J
A. Burrows and J. Goshy, A Theory of Supernova Ex- plosions, ApJ Lett. 416, L75 (1993)
1993
-
[22]
B. M¨ uller, H.-T. Janka, and A. Heger, New Two- dimensional Models of Supernova Explosions by the Neutrino-heating Mechanism: Evidence for Different Instability Regimes in Collapsing Stellar Cores, Astro- phys. J. 761, 72 (2012), arXiv:1205.7078 [astro-ph.SR]
- [23]
- [24]
- [25]
-
[26]
K. N. Yakunin, A. Mezzacappa, P. Marronetti, S. Yoshida, S. W. Bruenn, W. R. Hix, E. J. Lentz, O. E. Bronson Messer, J. A. Harris, E. Endeve, J. M. Blondin, 11 and E. J. Lingerfelt, Gravitational wave signatures of ab initio two-dimensional core collapse supernova explosion models for 12 -25 M ⊙ stars, Phys. Rev. D 92, 084040 (2015), arXiv:1505.05824 [ast...
-
[27]
H. Andresen, B. M¨ uller, E. M¨ uller, and H. T. Janka, Gravitational wave signals from 3D neutrino hydrody- namics simulations of core-collapse supernovae, MN- RAS 468, 2032 (2017), arXiv:1607.05199 [astro-ph.HE]
-
[28]
A. Mezzacappa, P. Marronetti, R. E. Landfield, E. J. Lentz, R. D. Murphy, W. Raphael Hix, J. A. Harris, S. W. Bruenn, J. M. Blondin, O. E. Bronson Messer, J. Casanova, and L. L. Kronzer, Core collapse super- nova gravitational wave emission for progenitors of 9.6, 15, and 25M ⊙, Phys. Rev. D 107, 043008 (2023), arXiv:2208.10643 [astro-ph.SR]
- [29]
- [30]
- [31]
- [32]
- [33]
-
[34]
B. M¨ uller, T. Melson, A. Heger, and H.-T. Janka, Su- pernova simulations from a 3D progenitor model - Im- pact of perturbations and evolution of explosion proper- ties, MNRAS 472, 491 (2017), arXiv:1705.00620 [astro- ph.SR]
-
[35]
H. Nagakura, K. Takahashi, and Y. Yamamoto, On the importance of progenitor asymmetry to shock revival in core-collapse supernovae, MNRAS 483, 208 (2019), arXiv:1811.05515 [astro-ph.HE]
-
[36]
R. Kazeroni and E. Abdikamalov, The impact of pro- genitor asymmetries on the neutrino-driven convection in core-collapse supernovae, MNRAS 494, 5360 (2020), arXiv:1911.08819 [astro-ph.SR]
-
[37]
D. Vartanyan, M. S. B. Coleman, and A. Burrows, The collapse and three-dimensional explosion of three- dimensional massive-star supernova progenitor models, MNRAS 510, 4689 (2022), arXiv:2109.10920 [astro- ph.SR]
- [38]
- [39]
-
[40]
T. Foglizzo, L. Scheck, and H. T. Janka, Neutrino-driven Convection versus Advection in Core-Collapse Super- novae, Astrophys. J. 652, 1436 (2006), arXiv:astro- ph/0507636 [astro-ph]
- [41]
- [42]
- [43]
-
[44]
B. M¨ uller and H.-T. Janka, Non-radial instabilities and progenitor asphericities in core-collapse supernovae, MNRAS 448, 2141 (2015), arXiv:1409.4783 [astro- ph.SR]
-
[45]
S. W. Bruenn, E. J. Lentz, W. R. Hix, A. Mezzacappa, J. A. Harris, O. E. B. Messer, E. Endeve, J. M. Blondin, M. A. Chertkow, E. J. Lingerfelt, P. Marronetti, and K. N. Yakunin, The Development of Explosions in Ax- isymmetric Ab Initio Core-collapse Supernova Simula- tions of 12-25 M Stars, Astrophys. J. 818, 123 (2016), arXiv:1409.5779 [astro-ph.SR]
- [46]
-
[47]
C. D. Ott, E. Abdikamalov, E. O’Connor, C. Reiss- wig, R. Haas, P. Kalmus, S. Drasco, A. Burrows, and E. Schnetter, Correlated gravitational wave and neu- trino signals from general-relativistic rapidly rotating iron core collapse, Phys. Rev. D 86, 024026 (2012), arXiv:1204.0512 [astro-ph.HE]
- [48]
-
[49]
S. Scheidegger, T. Fischer, S. C. Whitehouse, and M. Liebend¨ orfer, Gravitational waves from 3D MHD core collapse simulations, A&A 490, 231 (2008), arXiv:0709.0168 [astro-ph]
-
[50]
S. Shibagaki, T. Kuroda, K. Kotake, and T. Takiwaki, A new gravitational-wave signature of low-T/—W— in- stability in rapidly rotating stellar core collapse, MN- RAS 493, L138 (2020), arXiv:1909.09730 [astro-ph.HE]
- [51]
-
[52]
Mueller and H
E. Mueller and H. T. Janka, Gravitational radiation from convective instabilities in Type II supernova ex- plosions., A&A 317, 140 (1997)
1997
-
[53]
T. Takiwaki and K. Kotake, Anisotropic emission of neutrino and gravitational-wave signals from rapidly rotating core-collapse supernovae, MNRAS 475, L91 (2018), arXiv:1711.01905 [astro-ph.HE]
-
[54]
D. Vartanyan and A. Burrows, Gravitational Waves from Neutrino Emission Asymmetries in Core- 12 collapse Supernovae, Astrophys. J. 901, 108 (2020), arXiv:2007.07261 [astro-ph.HE]
- [55]
- [56]
-
[57]
O. Birnholtz and T. Piran, Gravitational wave memory from gamma ray bursts’ jets, Phys. Rev. D 87, 123007 (2013), arXiv:1302.5713 [astro-ph.HE]
- [58]
-
[59]
P. M¨ osta, S. Richers, C. D. Ott, R. Haas, A. L. Piro, K. Boydstun, E. Abdikamalov, C. Reisswig, and E. Schnetter, Magnetorotational Core-collapse Super- novae in Three Dimensions, ApJL 785, L29 (2014), arXiv:1403.1230 [astro-ph.HE]
-
[60]
M. Obergaulinger and M. ´A. Aloy, Magnetorota- tional core collapse of possible GRB progenitors - I. Explosion mechanisms, MNRAS 492, 4613 (2020), arXiv:1909.01105 [astro-ph.HE]
- [61]
-
[62]
Cusinato, M
M. Cusinato, M. Obergaulinger, M. ´A. Aloy, and J. A. Font, Resonant amplification of multimessenger emis- sion in rotating stellar core collapse, Physical Review Research 8, 013180 (2026)
2026
- [63]
-
[64]
Abdikamalov, G
E. Abdikamalov, G. Pagliaroli, and D. Radice, Grav- itational Waves from Core-Collapse Supernovae, in Handbook of Gravitational Wave Astronomy , edited by C. Bambi, S. Katsanevas, and K. D. Kokkotas (2022) p. 21
2022
-
[65]
Casallas-Lagos, J
A. Casallas-Lagos, J. M. Antelis, C. Moreno, M. Zano- lin, A. Mezzacappa, and M. J. Szczepa´ nczyk, Charac- terizing the temporal evolution of the high-frequency gravitational wave emission for a core collapse super- nova with laser interferometric data: A neural network approach, Phys. Rev. D 108, 084027 (2023)
2023
- [66]
- [67]
-
[68]
J. Powell, A. Iess, M. Llorens-Monteagudo, M. Ober- gaulinger, B. M¨ uller, A. Torres-Forn´ e, E. Cuoco, and J. A. Font, Determining the core-collapse super- nova explosion mechanism with current and future gravitational-wave observatories, Phys. Rev. D 109, 063019 (2024), arXiv:2311.18221 [astro-ph.HE]
-
[69]
E. Abdikamalov, S. Gossan, A. M. DeMaio, and C. D. Ott, Measuring the angular momentum distribution in core-collapse supernova progenitors with gravitational waves, Phys. Rev. D90, 044001 (2014), arXiv:1311.3678 [astro-ph.SR]
- [70]
-
[71]
M.-A. Bizouard, P. Maturana-Russel, A. Torres-Forn´ e, M. Obergaulinger, P. Cerd´ a-Dur´ an, N. Christensen, J. A. Font, and R. Meyer, Inference of protoneutron star properties from gravitational-wave data in core- collapse supernovae, Phys. Rev. D 103, 063006 (2021), arXiv:2012.00846 [gr-qc]
-
[72]
T. Bruel, M.-A. Bizouard, M. Obergaulinger, P. Maturana-Russel, A. Torres-Forn´ e, P. Cerd´ a-Dur´ an, N. Christensen, J. A. Font, and R. Meyer, Inference of protoneutron star properties in core-collapse su- pernovae from a gravitational-wave detector network, Phys. Rev. D 107, 083029 (2023), arXiv:2301.10019 [astro-ph.HE]
-
[73]
P. Cerd´ a-Dur´ an, N. DeBrye, M. A. Aloy, J. A. Font, and M. Obergaulinger, Gravitational Wave Signatures in Black Hole Forming Core Collapse, ApJL 779, L18 (2013), arXiv:1310.8290 [astro-ph.SR]
- [74]
-
[75]
S. Shibagaki, T. Kuroda, K. Kotake, and T. Taki- waki, Characteristic time variability of gravitational- wave and neutrino signals from three-dimensional simu- lations of non-rotating and rapidly rotating stellar core collapse, MNRAS 502, 3066 (2021), arXiv:2010.03882 [astro-ph.HE]
-
[76]
A. Burrows, D. Vartanyan, and T. Wang, Black Hole Formation Accompanied by the Supernova Explosion of a 40 M ⊙ Progenitor Star, Astrophys. J. 957, 68 (2023), arXiv:2308.05798 [astro-ph.SR]
-
[77]
J. Powell and B. M¨ uller, Gravitational waves from core-collapse supernovae with no electromagnetic coun- terparts, arXiv e-prints , arXiv:2506.03581 (2025), arXiv:2506.03581 [astro-ph.HE]
-
[78]
O. Eggenberger Andersen, E. O’Connor, H. Andresen, A. da Silva Schneider, and S. M. Couch, Black Hole Supernovae, Their Equation of State Dependence, and Ejecta Composition, Astrophys. J. 980, 53 (2025), arXiv:2411.11969 [astro-ph.HE]
- [79]
-
[80]
T. Kuroda and M. Shibata, Failed supernova simula- tions beyond black hole formation, MNRAS 526, 152 (2023), arXiv:2307.06192 [astro-ph.HE]
discussion (0)
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