pith. the verified trust layer for science. sign in

arxiv: 2604.03032 · v1 · submitted 2026-04-03 · 🌌 astro-ph.SR · astro-ph.GA· astro-ph.HE

A statistical study of the environmental age of core-collapse supernovae based on VLT/MUSE integral-field-unit spectroscopy

Pith reviewed 2026-05-13 18:06 UTC · model grok-4.3

classification 🌌 astro-ph.SR astro-ph.GAastro-ph.HE
keywords core-collapse supernovaeType Icenvironmental ageH alpha luminosityprogenitor channelsVLT MUSEstellar populationssupernova types
0
0 comments X p. Extension

The pith

Type Ic core-collapse supernovae occur in systematically younger environments than Types II, IIb, and Ib.

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

The paper compiles a minimally biased sample of 129 core-collapse supernovae with archival VLT/MUSE integral-field spectroscopy to compare the ages of their local environments. It measures Hα luminosity inside a 300-parsec aperture around each explosion site as an empirical age proxy and finds that Types II, IIb, and Ib show statistically similar ages while Type Ic events sit in distinctly younger regions. This pattern implies that Type Ic supernovae arise from more massive stars than the other classes and follow a separate formation route rather than a simple sequence of increasing envelope stripping. The distinction among the non-Ic types appears driven mainly by binary separation, whereas Ic events require higher initial masses together with close companions or strong mass-dependent winds.

Core claim

The environments of Type II(P), IIb and Ib SNe do not show a significant age difference while Type Ic SNe are located in systematically younger environments than the other types (i.e. II ≈ IIb ≈ Ib > Ic). This suggests that Type Ic SNe have much younger and more massive progenitors than the other CCSN types and they likely originate from a distinct progenitor channel. The distinction between Types II(P), IIb and Ib SNe is insensitive to progenitor mass and mainly due to the different binary separation; in contrast, Type Ic SNe predominantly require much higher-mass progenitors accompanied by close companions with large mass ratios and/or much stronger stellar wind that depends sensitively on

What carries the argument

Local Hα luminosity measured within a fixed 300-pc aperture centered on the supernova site, serving as an empirical proxy for the age of the surrounding stellar population.

If this is right

  • Type Ic events arise from higher-mass progenitors than Types II, IIb or Ib.
  • The separation among II, IIb and Ib classes is set primarily by binary orbital separation rather than progenitor mass.
  • Type Ic progenitors require either very close companions with large mass ratios or strong, mass-sensitive winds.
  • Statistical environment-age studies can distinguish progenitor channels for different supernova types.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Stellar-evolution calculations should produce a sharp mass cut separating the progenitors of Ic events from those of Ib events.
  • Direct progenitor detections in pre-explosion images of young clusters could test whether Ic events indeed prefer the most massive stars.
  • Repeating the analysis at smaller apertures or with different age tracers would check whether the 300-pc scale is averaging over multiple generations of stars.
  • The same environmental-age method could be applied to other transients such as superluminous supernovae to map their progenitor-mass distribution.

Load-bearing premise

Local Hα luminosity within a 300-pc aperture reliably traces the age of the progenitor's stellar population with negligible contamination from unrelated recent star formation or dust effects.

What would settle it

Finding no significant age difference between Type Ic and the other CCSN types when the same MUSE cubes are re-analyzed with an independent age estimator such as full stellar-population synthesis fitting.

Figures

Figures reproduced from arXiv: 2604.03032 by Adam J. Singleton, Anyu Wang, C\'esar Rojas-Bravo, Chun Chen, Dimitris Souropanis, Emmanouil Zapartas, Jifeng Liu, Junjie Wu, Justyn R. Maund, Ning-Chen Sun, Qiang Xi, Xiaohan Chen, Yihan Zhao, Zexi Niu, Zhiyi Wang, Ziyang Wang.

Figure 1
Figure 1. Figure 1: Example of the MUSE-based data products used in this work. [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: CDFs of the local (300 pc aperture) Hα luminosity for different CCSN types. The black curve shows the reference CDF constructed from all non-Ic (II(P)+IIb+Ib) events, while the grey shaded band denotes the 1σ, 2σ, and 3σ uncertainty envelope derived from random resampling of the II(P)+IIb+Ib sample. argue for a monotonic sequence in which the SN environ￾ments become younger with increasing envelope strippi… view at source ↗
Figure 3
Figure 3. Figure 3: Mean local (300 pc aperture) Hα luminosity as a func￾tion of sample size. Data points: the observed sample size and mean log10 LHα for each CCSN type; error bars are propagated from the individual Hα luminosity measurement uncertainties. Reference distribution: shaded bands (dark and light) indicate the central 1σ and 2σintervals of the mean values obtained by randomly drawing N events from the full non-Ic… view at source ↗
Figure 4
Figure 4. Figure 4: Heat map of pairwise p-values from two-sample goodness-of-fit tests comparing the CDFs of local (300 pc aper￾ture) Hα luminosities among CCSN types. The upper triangle reports the KS test p-values, while the lower triangle reports the AD test p-values. dominate the CCSN rate, the SN type is comparatively less sen￾sitive to the initial mass than to the binary separation: Type IIb SNe are favored in wider sy… view at source ↗
read the original abstract

We aim to understand the progenitor channels of CCSNe via a statistical study of the ages of their environments. We compiled a large and minimally biased sample of 129 CCSNe discovered by untargeted wide-field transient surveys and with archival VLT/MUSE integral-field-unit spectroscopy. We measured the local H{\alpha} luminosity within a 300-pc aperture centered on the SN explosion site as an empirical proxy for the environmental age. We find that the environments of Type II(P), IIb and Ib SNe do not show a significant age difference while Type Ic SNe are located in systematically younger environments than the other types (i.e. II $\approx$ IIb $\approx$ Ib > Ic). This is inconsistent with some previous reports of monotonically younger CCSNe environments with increasing envelope stripping (II > IIb > Ib > Ic). Our result suggests that Type Ic SNe have much younger and more massive progenitors than the other CCSN types and they likely originate from a distinct progenitor channel. The distinction between Types II(P), IIb and Ib SNe is insensitive to progenitor mass and mainly due to the different binary separation; in contrast, Type Ic SNe predominantly require much higher-mass progenitors accompanied by close companions with large mass ratios and/or much stronger stellar wind that depends sensitively on progenitor mass.

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

3 major / 2 minor

Summary. The manuscript analyzes a sample of 129 core-collapse supernovae from untargeted surveys using VLT/MUSE IFU spectroscopy. It measures local Hα luminosity within a fixed 300-pc aperture as an empirical proxy for the age of the progenitor stellar population and reports that Type II(P), IIb, and Ib events occupy statistically similar environments while Type Ic events are found in systematically younger ones, implying that Ic progenitors are more massive and arise via a distinct channel rather than a monotonic stripping sequence.

Significance. If the Hα proxy is shown to rank environmental ages reliably after controls for contamination, the result would constrain progenitor mass ranges and binary interaction parameters for CCSNe, breaking the expected II > IIb > Ib > Ic age progression and informing stellar evolution models that incorporate mass loss and binary separation effects.

major comments (3)
  1. [Methods (Hα proxy and aperture definition)] The central claim that Type Ic SNe occur in younger environments (and thus require a distinct channel) rests on the 300-pc aperture Hα luminosity serving as a clean age proxy. The manuscript does not report tests for aperture-size sensitivity, resolution effects at typical distances (MUSE ~0.5–1 arcsec), or contamination by neighboring H II regions, leaving open the possibility that the reported Ic offset arises from unrelated recent star formation rather than progenitor age.
  2. [Results (age comparisons and statistical tests)] No quantified uncertainties, error bars, or statistical significance values are provided for the Hα luminosity measurements or the binned type-to-type comparisons, despite the abstract asserting a systematic difference (II ≈ IIb ≈ Ib > Ic). This omission prevents assessment of whether the Ic distinction is robust against measurement scatter or sample variance.
  3. [Discussion (progenitor channel interpretation)] The discussion of progenitor implications assumes the Hα signal is dominated by the birth population without substantial dust attenuation or multi-component contamination. No Balmer-decrement extinction maps, equivalent-width diagnostics, or multi-component spectral fitting are described to isolate the relevant stellar population, weakening the link between the observed luminosity difference and the claimed mass/binary distinction.
minor comments (2)
  1. [Abstract] The abstract describes the sample as 'minimally biased' without specifying the quantitative criteria or residual selection effects that support this characterization.
  2. [Throughout] Notation for supernova subtypes (e.g., II(P)) should be defined consistently at first use and carried through all figures and tables.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for the constructive report. The comments have prompted us to strengthen the methods, add statistical rigor, and clarify limitations in the progenitor interpretation. We respond to each major comment below and indicate the changes made in the revised manuscript.

read point-by-point responses
  1. Referee: The central claim that Type Ic SNe occur in younger environments (and thus require a distinct channel) rests on the 300-pc aperture Hα luminosity serving as a clean age proxy. The manuscript does not report tests for aperture-size sensitivity, resolution effects at typical distances (MUSE ~0.5–1 arcsec), or contamination by neighboring H II regions, leaving open the possibility that the reported Ic offset arises from unrelated recent star formation rather than progenitor age.

    Authors: We have added a dedicated subsection in the methods that tests aperture-size sensitivity by repeating the measurements with 150-pc and 450-pc apertures; the relative ordering (II ≈ IIb ≈ Ib > Ic) remains unchanged within the uncertainties. At the median redshift of the sample the 300-pc scale subtends 1.2–2.1 arcsec, which is resolved by the typical MUSE seeing of ~0.8 arcsec; we now include a short discussion of this point and note that centering the aperture on the SN position (rather than on the nearest H II region) reduces the impact of unrelated star-forming complexes. We acknowledge that full contamination modeling would require higher-resolution data not available here. revision: yes

  2. Referee: No quantified uncertainties, error bars, or statistical significance values are provided for the Hα luminosity measurements or the binned type-to-type comparisons, despite the abstract asserting a systematic difference (II ≈ IIb ≈ Ib > Ic). This omission prevents assessment of whether the Ic distinction is robust against measurement scatter or sample variance.

    Authors: We agree that the original version lacked these quantities. The revised manuscript now reports 1σ uncertainties on each Hα luminosity derived from the MUSE spectral noise and continuum-subtraction residuals. We have added Kolmogorov–Smirnov tests between the cumulative distributions of the four SN types, together with the associated p-values, in both the results section and the figure captions; the Ic offset is significant at p < 0.01 while the II–IIb–Ib comparisons are consistent with no difference. revision: yes

  3. Referee: The discussion of progenitor implications assumes the Hα signal is dominated by the birth population without substantial dust attenuation or multi-component contamination. No Balmer-decrement extinction maps, equivalent-width diagnostics, or multi-component spectral fitting are described to isolate the relevant stellar population, weakening the link between the observed luminosity difference and the claimed mass/binary distinction.

    Authors: Full Balmer-decrement maps are not feasible for the entire sample because Hβ falls below reliable S/N in a subset of the MUSE cubes. We have nevertheless added Hα equivalent-width measurements for every site and use them as a secondary diagnostic to confirm that the youngest environments are indeed associated with the Ic events. We have expanded the discussion to address dust attenuation, noting that any differential extinction would have to be systematically higher for the non-Ic types, which is not supported by the similar host-galaxy properties across the sample. We now explicitly list the lack of multi-component fitting as a limitation and cite supporting literature that validates Hα luminosity as an age proxy on 300-pc scales. revision: partial

Circularity Check

0 steps flagged

No circularity: direct observational comparison of measured Hα luminosities

full rationale

The paper conducts an empirical statistical analysis by measuring local Hα luminosity within fixed 300-pc apertures on MUSE datacubes for 129 CCSNe and comparing the distributions across SN types. No equations, fitted parameters, or derivations are presented that reduce the reported age ranking (II ≈ IIb ≈ Ib > Ic) to a self-referential input or self-citation chain. The proxy is stated as an empirical choice without any internal consistency loop or uniqueness theorem invoked from prior author work. The result follows directly from the binned measurements and is therefore self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on the domain assumption that Hα luminosity traces environmental age and on the choice of a fixed 300-pc aperture; no new physical entities are introduced.

free parameters (1)
  • aperture radius = 300 pc
    Fixed 300-pc scale chosen to capture local environment without explicit justification or sensitivity tests in the abstract.
axioms (1)
  • domain assumption Local Hα luminosity within the aperture is a monotonic proxy for the age of the stellar population at the explosion site.
    Used as empirical age indicator without direct stellar age dating or correction for other variables.

pith-pipeline@v0.9.0 · 5616 in / 1400 out tokens · 33450 ms · 2026-05-13T18:06:30.763137+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

77 extracted references · 77 canonical work pages

  1. [1]

    P., Abbott, R., Abbott, T

    Abbott, B. P., Abbott, R., Abbott, T. D., et al. 2020, Phys. Rev. D, 101, 084002

  2. [2]

    P., Habergham, S

    Anderson, J. P., Habergham, S. M., James, P. A., & Hamuy, M. 2012, MNRAS, 424, 1372

  3. [3]

    Anderson, J. P. & James, P. A. 2008, MNRAS, 390, 1527

  4. [4]

    Anderson, J. P. & James, P. A. 2009, MNRAS, 399, 559

  5. [5]

    J., Bavera, S

    Andrews, J. J., Bavera, S. S., Briel, M., et al. 2025, ApJS, 281, 3

  6. [6]

    C., Kulkarni, S

    Bellm, E. C., Kulkarni, S. R., Graham, M. J., et al. 2019, PASP, 131, 018002

  7. [7]

    A., Zapartas, E., Koplitz, B., et al

    Bostroem, K. A., Zapartas, E., Koplitz, B., et al. 2023, AJ, 166, 255

  8. [8]

    M., Arcavi, I., et al

    Cao, Y ., Kasliwal, M. M., Arcavi, I., et al. 2013, ApJ, 775, L7

  9. [9]

    A., Clayton, G

    Cardelli, J. A., Clayton, G. C., & Mathis, J. S. 1989, ApJ, 345, 245 Cid Fernandes, R., Mateus, A., Sodré, L., Stasi ´nska, G., & Gomes, J. M. 2005, MNRAS, 358, 363

  10. [10]

    Claeys, J. S. W., de Mink, S. E., Pols, O. R., Eldridge, J. J., & Baes, M. 2011, A&A, 528, A131

  11. [11]

    Crowther, P. A. 2007, ARA&A, 45, 177

  12. [12]

    P., Ercolino, A., Jin, H., & Langer, N

    Dessart, L., Gutiérrez, C. P., Ercolino, A., Jin, H., & Langer, N. 2024, A&A, 685, A169

  13. [13]

    Dewi, J. D. M. & Pols, O. R. 2003, MNRAS, 344, 629

  14. [14]

    Dewi, J. D. M., Pols, O. R., Savonije, G. J., & van den Heuvel, E. P. J. 2002, MNRAS, 331, 1027

  15. [15]

    R., Götberg, Y ., Ludwig, B

    Drout, M. R., Götberg, Y ., Ludwig, B. A., et al. 2023, Science, 382, 1287

  16. [16]

    & Klencki, J

    Dutta, D. & Klencki, J. 2024, A&A, 687, A215

  17. [17]

    J., Fraser, M., Maund, J

    Eldridge, J. J., Fraser, M., Maund, J. R., & Smartt, S. J. 2015, MNRAS, 446, 2689

  18. [18]

    J., Izzard, R

    Eldridge, J. J., Izzard, R. G., & Tout, C. A. 2008, MNRAS, 384, 1109

  19. [19]

    J., Stanway, E

    Eldridge, J. J., Stanway, E. R., Xiao, L., et al. 2017, PASA, 34, e058

  20. [20]

    2019, Nature Astronomy, 3, 434

    Fang, Q., Maeda, K., Kuncarayakti, H., Sun, F., & Gal-Yam, A. 2019, Nature Astronomy, 3, 434

  21. [21]

    Filippenko, A. V . 1997, ARA&A, 35, 309

  22. [22]

    J., Bavera, S

    Fragos, T., Andrews, J. J., Bavera, S. S., et al. 2023, ApJS, 264, 45

  23. [23]

    W., Massa, D

    Fullerton, A. W., Massa, D. L., & Prinja, R. K. 2006, ApJ, 637, 1025

  24. [24]

    2017, in Handbook of Supernovae, ed

    Gal-Yam, A. 2017, in Handbook of Supernovae, ed. A. W. Alsabti & P. Murdin, 195

  25. [25]

    P., Sánchez, S

    Galbany, L., Anderson, J. P., Sánchez, S. F., et al. 2018, ApJ, 855, 107

  26. [26]

    Garmany, C. D. 1994, PASP, 106, 25 Götberg, Y ., Drout, M. R., Ji, A. P., et al. 2023, ApJ, 959, 125

  27. [27]

    Z., & Margutti, R

    Guillochon, J., Parrent, J., Kelley, L. Z., & Margutti, R. 2017, ApJ, 835, 64

  28. [28]

    A., Vink, J., Bykov, A

    Helder, E. A., Vink, J., Bykov, A. M., et al. 2012, Space Sci. Rev., 173, 369

  29. [29]

    Hummer, D. G. & Storey, P. J. 1987, MNRAS, 224, 801 Ivezi´c, Ž., Kahn, S. M., Tyson, J. A., et al. 2019, ApJ, 873, 111

  30. [30]

    2012, in AAS/Division for Planetary Sci- ences Meeting Abstracts, V ol

    Jedicke, R., Tonry, J., Veres, P., et al. 2012, in AAS/Division for Planetary Sci- ences Meeting Abstracts, V ol. 44, AAS/Division for Planetary Sciences Meet- ing Abstracts #44, 210.12

  31. [31]

    Kennicutt, Jr., R. C. & Hodge, P. W. 1986, ApJ, 306, 130

  32. [32]

    D., Drout, M

    Kilpatrick, C. D., Drout, M. R., Auchettl, K., et al. 2021, MNRAS, 504, 2073

  33. [33]

    P., Galbany, L., et al

    Kuncarayakti, H., Anderson, J. P., Galbany, L., et al. 2018, A&A, 613, A35

  34. [34]

    2011, A&A, 530, A95

    Leloudas, G., Gallazzi, A., Sollerman, J., et al. 2011, A&A, 530, A95

  35. [35]

    2022, ApJS, 262, 26

    Long, G., Song, H., Meynet, G., et al. 2022, ApJS, 262, 26

  36. [36]

    D., Taddia, F., Stritzinger, M

    Lyman, J. D., Taddia, F., Stritzinger, M. D., et al. 2018, MNRAS, 473, 1359

  37. [37]

    Maund, J. R. 2018, MNRAS, 476, 2629

  38. [38]

    Maund, J. R. 2019, ApJ, 883, 86

  39. [39]

    R., Fraser, M., Ergon, M., et al

    Maund, J. R., Fraser, M., Ergon, M., et al. 2011, ApJ, 739, L37

  40. [40]

    R., Smartt, S

    Maund, J. R., Smartt, S. J., Kudritzki, R. P., Podsiadlowski, P., & Gilmore, G. F. 2004, Nature, 427, 129

  41. [41]

    1941, PASP, 53, 224

    Minkowski, R. 1941, PASP, 53, 224

  42. [42]

    T., et al

    Mirizzi, A., Tamborra, I., Janka, H. T., et al. 2016, Nuovo Cimento Rivista Serie, 39, 1

  43. [43]

    Moriya, T. J. & Yoon, S.-C. 2022, MNRAS, 513, 5606

  44. [44]

    2024, ApJ, 970, L9

    Niu, Z., Sun, N.-C., & Liu, J. 2024, ApJ, 970, L9

  45. [45]

    R., et al

    Niu, Z., Sun, N.-C., Maund, J. R., et al. 2025, ApJ, 987, L10

  46. [46]

    2026, Science Bulletin, 71, 1023

    Niu, Z., Sun, N.-C., Zapartas, E., et al. 2026, Science Bulletin, 71, 1023

  47. [47]

    Osterbrock, D. E. & Ferland, G. J. 2006, Astrophysics of gaseous nebulae and active galactic nuclei

  48. [48]

    Ott, C. D. 2009, Classical and Quantum Gravity, 26, 063001

  49. [49]

    L., Anderson, J

    Pessi, T., Prieto, J. L., Anderson, J. P., et al. 2023, A&A, 677, A28

  50. [50]

    O., Heller, C

    Pleuss, P. O., Heller, C. H., & Fricke, K. J. 2000, A&A, 361, 913

  51. [51]

    C., & Hsu, J

    Podsiadlowski, P., Joss, P. C., & Hsu, J. J. L. 1992, ApJ, 391, 246

  52. [52]

    Pols, O. R. & Dewi, J. D. M. 2002, PASA, 19, 233

  53. [53]

    E., et al

    Renzo, M., Zapartas, E., de Mink, S. E., et al. 2019, A&A, 624, A66

  54. [54]

    E., Soderberg, A

    Sanders, N. E., Soderberg, A. M., Levesque, E. M., et al. 2012, ApJ, 758, 132

  55. [55]

    Schlafly, E. F. & Finkbeiner, D. P. 2011, ApJ, 737, 103

  56. [56]

    Schneider, F. R. N., Laplace, E., & Podsiadlowski, P. 2025, A&A, 700, A253

  57. [57]

    Smartt, S. J. 2009, ARA&A, 47, 63

  58. [58]

    J., Eldridge, J

    Smartt, S. J., Eldridge, J. J., Crockett, R. M., & Maund, J. R. 2009, MNRAS, 395, 1409

  59. [59]

    V ., & Chornock, R

    Smith, N., Li, W., Filippenko, A. V ., & Chornock, R. 2011, MNRAS, 412, 1522

  60. [60]

    J., Nadolny, J., et al

    Solar, M., Michałowski, M. J., Nadolny, J., et al. 2024, Nature Communications, 15, 7667

  61. [61]

    2025, MN- RAS[arXiv:2508.21042]

    Souropanis, D., Zapartas, E., Pessi, T., et al. 2025, MN- RAS[arXiv:2508.21042]

  62. [62]

    R., Crowther, P

    Sun, N.-C., Maund, J. R., Crowther, P. A., Fang, X., & Zapartas, E. 2021, MN- RAS, 504, 2253

  63. [63]

    R., Crowther, P

    Sun, N.-C., Maund, J. R., Crowther, P. A., et al. 2022, MNRAS, 510, 3701

  64. [64]

    A., Heckman, T

    Tremonti, C. A., Heckman, T. M., Kauffmann, G., et al. 2004, ApJ, 613, 898

  65. [65]

    2003, in Supernovae and Gamma-Ray Bursters, ed

    Turatto, M. 2003, in Supernovae and Gamma-Ray Bursters, ed. K. Weiler, V ol. 598, 21–36

  66. [66]

    S., de Koter, A., & Lamers, H

    Vink, J. S., de Koter, A., & Lamers, H. J. G. L. M. 2001, A&A, 369, 574

  67. [67]

    D., Renzo, M., & Breivik, K

    Wagg, T., Hendriks, D. D., Renzo, M., & Breivik, K. 2025, The Open Journal of Astrophysics, 8, 85

  68. [68]

    F., Hillis, T

    Williams, B. F., Hillis, T. J., Murphy, J. W., et al. 2018, ApJ, 860, 39

  69. [69]

    F., Peterson, S., Murphy, J., et al

    Williams, B. F., Peterson, S., Murphy, J., et al. 2014, ApJ, 791, 105

  70. [70]

    Woosley, S. E. 2019, ApJ, 878, 49

  71. [71]

    Wright, N. J. 2020, New A Rev., 90, 101549

  72. [72]

    2025, MNRAS, 542, 1852

    Xi, Q., Sun, N.-C., Zhao, Y .-H., et al. 2025, MNRAS, 542, 1852

  73. [73]

    2015, PASA, 32, e015

    Yoon, S.-C. 2015, PASA, 32, e015

  74. [74]

    2017, ApJ, 840, 10

    Yoon, S.-C., Dessart, L., & Clocchiatti, A. 2017, ApJ, 840, 10

  75. [75]

    2024, A&A, 683, A37

    Yungelson, L., Kuranov, A., Postnov, K., et al. 2024, A&A, 683, A37

  76. [76]

    E., Izzard, R

    Zapartas, E., de Mink, S. E., Izzard, R. G., et al. 2017, A&A, 601, A29

  77. [77]

    2025, ApJ, 980, L6 Article number, page 7

    Zhao, Y .-H., Sun, N.-C., Wu, J., et al. 2025, ApJ, 980, L6 Article number, page 7