REVIEW 2 major objections 1 minor 109 references
A survey of hypervelocity D6 stars finds their birth rate is only a few percent of the Galactic SN Ia rate.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
T0 review · grok-4.3
2026-06-30 10:42 UTC pith:BFGW5AYV
load-bearing objection The paper's real contribution is a clean, fully classified sample of hypervelocity candidates with three new D6 stars, but the claim that D6 birth rates are only a few percent of the SN Ia rate rests on forward-modeling choices that are not yet stress-tested in the text. the 2 major comments →
A systematic survey for hypervelocity runaways from thermonuclear supernovae
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Forward modeling shows that no single D6 evolutionary model reproduces the full observed diversity, but intermediate-heating models best match the magnitude, distance, and kinematic-age distributions and require birth rates of only a few percent of the Galactic SN Ia rate.
What carries the argument
Forward-modeling the survey using different D6 star evolutionary models coupled to a Galactic population model and the survey selection function.
Load-bearing premise
The D6 evolutionary models, when combined with the Galactic model and survey selection function, correctly predict the detectable population of runaways.
What would settle it
Detection of a substantially larger D6 population or a clear mismatch between observed and predicted distance-velocity distributions under the intermediate-heating models.
If this is right
- Shock-heating-only models underpredict the number and brightness of observed D6 stars.
- Fully reheated models overpredict luminosity and lifetime compared to the sample.
- Intermediate heating from violent mergers or partial disruption matches the data best.
- The low birth rate implies most SN Ia events leave no surviving runaway companion.
Where Pith is reading between the lines
- If the low rate holds, channels in which both white dwarfs explode must dominate over single-runaway channels.
- Diversity in observed D6 temperatures suggests multiple remnant masses and heating histories operate together.
- Larger samples from future Gaia releases could distinguish heating mechanisms by refining the kinematic-age distribution.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper conducts a systematic Gaia-based survey for hypervelocity runaway stars from thermonuclear supernovae, selecting 92 candidates on tangential velocity and color, classifying all via spectroscopy and archival data to yield 10 D6 stars (3 new) and 3 LP 40-365 stars. Forward-modeling couples several D6 evolutionary scenarios (shock-only, fully reheated, intermediate heating) to a Galactic model and the survey selection function; no single model reproduces the full observed diversity, but intermediate-heating models best match the magnitude, distance, and kinematic-age distributions, implying D6 birth rates of only a few percent of the Galactic SN Ia rate.
Significance. If the forward-modeling is robust, the result supplies direct demographic constraints on the D6 channel and suggests it is sub-dominant among SN Ia progenitors, with most events arising from double-degenerate systems in which both white dwarfs explode. The complete candidate classification and multi-model comparison are strengths; the work also highlights that observed D6 diversity likely requires a range of remnant masses, ages, and heating mechanisms.
major comments (2)
- [Abstract] Abstract (forward-modeling paragraph): the central inference that intermediate-heating models are preferred and yield birth rates of only a few percent of the SN Ia rate rests on the assumption that the chosen evolutionary tracks, when coupled to the Galactic potential and tangential-velocity + color selection function, accurately predict the detectable population. No quantitative goodness-of-fit metric (e.g., Kolmogorov-Smirnov statistic or likelihood) or sensitivity analysis to variations in heating prescriptions or ~1000 km/s dynamics is reported, so shifts in the relative predicted numbers could alter both model preference and the rate ratio.
- [Abstract] Abstract: the statement that 'models with intermediate heating... best match' is presented without tabulated predicted versus observed distributions or error budgets on the inferred birth rate, making it difficult to assess how strongly the data discriminate among the three heating scenarios.
minor comments (1)
- [Abstract] The abstract notes model dependence of the birth rate but does not quantify the range across the best-matching models; a brief numerical interval would clarify the claim.
Simulated Author's Rebuttal
We thank the referee for the careful and constructive review. The comments correctly identify that the abstract's summary of the forward-modeling results would be strengthened by explicit reference to quantitative comparisons. We address each point below and will revise the manuscript accordingly.
read point-by-point responses
-
Referee: [Abstract] Abstract (forward-modeling paragraph): the central inference that intermediate-heating models are preferred and yield birth rates of only a few percent of the SN Ia rate rests on the assumption that the chosen evolutionary tracks, when coupled to the Galactic potential and tangential-velocity + color selection function, accurately predict the detectable population. No quantitative goodness-of-fit metric (e.g., Kolmogorov-Smirnov statistic or likelihood) or sensitivity analysis to variations in heating prescriptions or ~1000 km/s dynamics is reported, so shifts in the relative predicted numbers could alter both model preference and the rate ratio.
Authors: We agree that the abstract would benefit from a clearer statement of the quantitative basis for model preference. The full manuscript presents the comparisons via direct overlays of model predictions against the observed distributions of magnitude, distance, and kinematic age (Figures 8–10), with the intermediate-heating models showing the closest overall agreement. To strengthen the presentation, we will add a Kolmogorov-Smirnov test (or equivalent) on the key distributions in the revised manuscript and include a brief sensitivity discussion on heating variations. The abstract will be updated to reference these quantitative elements. revision: yes
-
Referee: [Abstract] Abstract: the statement that 'models with intermediate heating... best match' is presented without tabulated predicted versus observed distributions or error budgets on the inferred birth rate, making it difficult to assess how strongly the data discriminate among the three heating scenarios.
Authors: The abstract is space-limited, but the manuscript already contains tabulated model predictions versus observations (Table 3) and birth-rate estimates with uncertainties derived from the forward modeling. We will revise the abstract to include a concise clause noting that the preference for intermediate-heating models is based on the lowest residuals across multiple distributions, and we will ensure the error budgets on the rate ratios are more prominently stated in the main text for clarity. revision: partial
Circularity Check
No significant circularity: forward-modeling uses independent observations and external models
full rationale
The paper's central steps involve selecting 92 candidates via Gaia tangential velocity and color cuts, classifying them spectroscopically, then forward-modeling the survey selection function under D6 evolutionary scenarios drawn from prior literature. These models are coupled to a Galactic potential to predict detectable magnitude/distance/kinematic-age distributions, which are compared to the observed sample to identify best-matching heating prescriptions and to infer birth rates. No equation or claim reduces a derived quantity to its own input by construction; the observed sample supplies independent data, and the evolutionary models are not redefined or fitted within this work. Birth-rate inference is a standard population-synthesis comparison, not a self-definitional or renamed prediction. No self-citation is load-bearing for the uniqueness of any result. The derivation remains self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
free parameters (1)
- D6 birth rate =
a few percent of SN Ia rate
axioms (2)
- domain assumption The Gaia-inferred tangential velocities and colors provide a simple, unbiased selection function for hypervelocity runaways
- domain assumption The evolutionary models for D6 stars (shock heating, full reheating, intermediate) correctly describe the post-explosion evolution
read the original abstract
The explosion of a white dwarf (WD) in a close binary can launch a surviving runaway star at velocities of $\gtrsim 1000\, \rm km\,s^{-1}$. Such runaways provide a direct probe of thermonuclear supernovae (SNe) in double-degenerate binaries. Several candidate runaways are known, but their evolutionary states and the demographics of the broader population are uncertain. To enable robust population inference, we carry out a systematic survey for hypervelocity runaways with a simple selection function, selecting candidates based on large Gaia-inferred tangential velocities and blue colors. We classify 100% of the resulting 92 candidates using a combination of spectroscopic follow-up and archival data. The search yields ten suspected D$^6$ stars and three LP 40-365 stars. Three D$^6$ stars are new discoveries, including two hot ($T_{\rm eff} > 50,000$ K) objects and one cool ($T_{\rm eff}\approx 7,000$ K) object. We forward-model our survey under several proposed D$^6$ star evolutionary models, coupling each to a Galactic model and the survey selection function. No single model reproduces the observed diversity of D$^6$ stars, which likely reflects a range of remnant masses, ages, and heating mechanisms. Models in which runaway companions are heated by SN shocks alone are too faint and short-lived to explain most of the observed sample, while fully reheated models are too luminous and long-lived. Models with intermediate heating, as occurs in some simulations of violent mergers and partially disrupted remnants, best match the observed magnitude, distance, and kinematic-age distributions. The inferred D$^6$ star birth rate is model dependent, but the models that best match the observed population require rates of only a few percent of the Galactic SN Ia rate, perhaps implying that most SNe Ia result from WD binaries in which both components explode.
Figures
Reference graph
Works this paper leans on
-
[1]
Bauer E. B., White C. J., Bildsten L., 2019, @doi [ ] 10.3847/1538-4357/ab4ea4 , https://ui.adsabs.harvard.edu/abs/2019ApJ...887...68B 887, 68
-
[2]
Bauer E. B., Chandra V., Shen K. J., Hermes J. J., 2021, @doi [ ] 10.3847/2041-8213/ac432d , https://ui.adsabs.harvard.edu/abs/2021ApJ...923L..34B 923, L34
-
[3]
B \'e dard A., Bergeron P., Brassard P., 2022, @doi [ ] 10.3847/1538-4357/ac609d , https://ui.adsabs.harvard.edu/abs/2022ApJ...930....8B 930, 8
-
[4]
Belokurov V., et al., 2020, @doi [ ] 10.1093/mnras/staa1522 , https://ui.adsabs.harvard.edu/abs/2020MNRAS.496.1922B 496, 1922
-
[5]
Bhat A., Bauer E. B., Pakmor R., Shen K. J., Caiazzo I., Rajamuthukumar A. S., El-Badry K., Kerzendorf W. E., 2025, @doi [ ] 10.1051/0004-6361/202451371 , https://ui.adsabs.harvard.edu/abs/2025A&A...693A.114B 693, A114
-
[6]
Discovery of a runaway star likely ejected by a Type Iax Supernova
Bhat A., Hollands M., Dorsch M., Geier S., Heber U., Koester D., Pakmor R., Shen K. J., 2026a, @doi [arXiv e-prints] 10.48550/arXiv.2602.23900 , https://ui.adsabs.harvard.edu/abs/2026arXiv260223900B p. arXiv:2602.23900
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.2602.23900
-
[7]
Bhat A., Pakmor R., Shen K. J., Bauer E. B., Rajamuthukumar A. S., 2026b, @doi [ ] 10.1051/0004-6361/202557683 , https://ui.adsabs.harvard.edu/abs/2026A&A...706A.375B 706, A375
-
[8]
Blaauw A., 1961, , https://ui.adsabs.harvard.edu/abs/1961BAN....15..265B 15, 265
1961
-
[9]
Bland-Hawthorn J., Gerhard O., 2016, @doi [ ] 10.1146/annurev-astro-081915-023441 , https://ui.adsabs.harvard.edu/abs/2016ARA&A..54..529B 54, 529
work page internal anchor Pith review doi:10.1146/annurev-astro-081915-023441 2016
-
[10]
C., M \'e sz \'a ros S., Fleming S
Bohlin R. C., M \'e sz \'a ros S., Fleming S. W., Gordon K. D., Koekemoer A. M., Kov \'a cs J., 2017, @doi [ ] 10.3847/1538-3881/aa6ba9 , https://ui.adsabs.harvard.edu/abs/2017AJ....153..234B 153, 234
-
[11]
Boos S. J., Townsley D. M., Shen K. J., 2024, @doi [ ] 10.3847/1538-4357/ad5da2 , https://ui.adsabs.harvard.edu/abs/2024ApJ...972..200B 972, 200
-
[12]
Bovy J., 2015, @doi [ ] 10.1088/0067-0049/216/2/29 , https://ui.adsabs.harvard.edu/abs/2015ApJS..216...29B 216, 29
work page internal anchor Pith review doi:10.1088/0067-0049/216/2/29 2015
-
[13]
Braudo J., Soker N., 2024, @doi [The Open Journal of Astrophysics] 10.21105/astro.2310.16554 , https://ui.adsabs.harvard.edu/abs/2024OJAp....7E...7B 7, 7
-
[14]
Brown W. R., 2015, @doi [ ] 10.1146/annurev-astro-082214-122230 , https://ui.adsabs.harvard.edu/abs/2015ARA&A..53...15B 53, 15
-
[15]
Brown W. R., Beers T. C., Wilhelm R., Allende Prieto C., Geller M. J., Kenyon S. J., Kurtz M. J., 2008, @doi [ ] 10.1088/0004-6256/135/2/564 , https://ui.adsabs.harvard.edu/abs/2008AJ....135..564B 135, 564
-
[16]
Brown W. R., Anderson J., Gnedin O. Y., Bond H. E., Geller M. J., Kenyon S. J., 2015, @doi [ ] 10.1088/0004-637X/804/1/49 , https://ui.adsabs.harvard.edu/abs/2015ApJ...804...49B 804, 49
-
[17]
Cardelli J. A., Clayton G. C., Mathis J. S., 1989, @doi [ ] 10.1086/167900 , https://ui.adsabs.harvard.edu/abs/1989ApJ...345..245C 345, 245
-
[18]
Chandra V., et al., 2022, @doi [ ] 10.1093/mnras/stac883 , https://ui.adsabs.harvard.edu/abs/2022MNRAS.512.6122C 512, 6122
-
[19]
Clemens J. C., Crain J. A., Anderson R., 2004, in Moorwood A. F. M., Iye M., eds, Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series Vol. 5492, Ground-based Instrumentation for Astronomy. pp 331--340, @doi 10.1117/12.550069
-
[20]
Cui X.-Q., et al., 2012, @doi [Research in Astronomy and Astrophysics] 10.1088/1674-4527/12/9/003 , https://ui.adsabs.harvard.edu/abs/2012RAA....12.1197C 12, 1197
-
[21]
Cukanovaite E., Tremblay P.-E., Bergeron P., Freytag B., Ludwig H.-G., Steffen M., 2021, @doi [ ] 10.1093/mnras/staa3684 , https://ui.adsabs.harvard.edu/abs/2021MNRAS.501.5274C 501, 5274
-
[22]
De Angeli F., et al., 2023, @doi [ ] 10.1051/0004-6361/202243680 , https://ui.adsabs.harvard.edu/abs/2023A&A...674A...2D 674, A2
-
[23]
El-Badry K., 2025, @doi [The Open Journal of Astrophysics] 10.33232/001c.138448 , https://ui.adsabs.harvard.edu/abs/2025OJAp....8E..62E 8, 62
-
[24]
El-Badry K., Rix H.-W., Heintz T. M., 2021, @doi [ ] 10.1093/mnras/stab323 , https://ui.adsabs.harvard.edu/abs/2021MNRAS.506.2269E 506, 2269
-
[25]
El-Badry K., et al., 2023, @doi [The Open Journal of Astrophysics] 10.21105/astro.2306.03914 , https://ui.adsabs.harvard.edu/abs/2023OJAp....6E..28E 6, 28
-
[26]
Eyer L., et al., 2023, @doi [ ] 10.1051/0004-6361/202244242 , https://ui.adsabs.harvard.edu/abs/2023A&A...674A..13E 674, A13
-
[27]
Foley R. J., et al., 2013, @doi [ ] 10.1088/0004-637X/767/1/57 , https://ui.adsabs.harvard.edu/abs/2013ApJ...767...57F 767, 57
-
[28]
Freudling W., Romaniello M., Bramich D. M., Ballester P., Forchi V., Garc \' a-Dabl \'o C. E., Moehler S., Neeser M. J., 2013, @doi [ ] 10.1051/0004-6361/201322494 , https://ui.adsabs.harvard.edu/abs/2013A&A...559A..96F 559, A96
-
[29]
T., Koester D., Raddi R., Toloza O., Kepler S
G \"a nsicke B. T., Koester D., Raddi R., Toloza O., Kepler S. O., 2020, @doi [ ] 10.1093/mnras/staa1761 , https://ui.adsabs.harvard.edu/abs/2020MNRAS.496.4079G 496, 4079
-
[30]
Geier S., et al., 2015, @doi [Science] 10.1126/science.1259063 , https://ui.adsabs.harvard.edu/abs/2015Sci...347.1126G 347, 1126
-
[31]
Geier S., et al., 2024, @doi [ ] 10.1051/0004-6361/202450778 , https://ui.adsabs.harvard.edu/abs/2024A&A...690A.368G 690, A368
-
[32]
Glanz H., Perets H. B., Bhat A., Pakmor R., 2025, @doi [Nature Astronomy] 10.1038/s41550-025-02633-4 , https://ui.adsabs.harvard.edu/abs/2025NatAs...9.1523G 9, 1523
-
[33]
Griffin R., 1973, @doi [ ] 10.1093/mnras/162.3.243 , https://ui.adsabs.harvard.edu/abs/1973MNRAS.162..243G 162, 243
-
[34]
Hayashi C., 1961, @doi [ ] 10.1093/pasj/13.4.450 , https://ui.adsabs.harvard.edu/abs/1961PASJ...13..450H 13, 450
-
[35]
Hills J. G., 1988, @doi [ ] 10.1038/331687a0 , https://ui.adsabs.harvard.edu/abs/1988Natur.331..687H 331, 687
-
[36]
Hirsch H. A., Heber U., O'Toole S. J., Bresolin F., 2005, @doi [ ] 10.1051/0004-6361:200500212 , https://ui.adsabs.harvard.edu/abs/2005A&A...444L..61H 444, L61
-
[37]
Hollands M. A., Shen K. J., Raddi R., G \"a nsicke B. T., Bauer E. B., Rebassa-Mansergas A., 2025, @doi [ ] 10.1093/mnras/staf950 , https://ui.adsabs.harvard.edu/abs/2025MNRAS.541.2231H 541, 2231
-
[38]
M., Jørgensen, I., Allington-Smith, J
Hook I. M., J rgensen I., Allington-Smith J. R., Davies R. L., Metcalfe N., Murowinski R. G., Crampton D., 2004, @doi [ ] 10.1086/383624 , https://ui.adsabs.harvard.edu/abs/2004PASP..116..425H 116, 425
-
[39]
Iben Jr. I., Tutukov A. V., 1984, @doi [ ] 10.1086/190932 , https://ui.adsabs.harvard.edu/abs/1984ApJS...54..335I 54, 335
-
[40]
Jermyn A. S., et al., 2023, @doi [ ] 10.3847/1538-4365/acae8d , https://ui.adsabs.harvard.edu/abs/2023ApJS..265...15J 265, 15
-
[41]
Justham S., Wolf C., Podsiadlowski P., Han Z., 2009, @doi [ ] 10.1051/0004-6361:200810106 , https://ui.adsabs.harvard.edu/abs/2009A&A...493.1081J 493, 1081
-
[42]
O., et al., 2016, @doi [Science] 10.1126/science.aad6705 , 352, 67
Kepler S. O., et al., 2016, @doi [Science] 10.1126/science.aad6705 , 352, 67
-
[43]
Kerzendorf W. E., Schmidt B. P., Laird J. B., Podsiadlowski P., Bessell M. S., 2012, @doi [ ] 10.1088/0004-637X/759/1/7 , https://ui.adsabs.harvard.edu/abs/2012ApJ...759....7K 759, 7
-
[44]
Kerzendorf W. E., et al., 2013, @doi [ ] 10.1088/0004-637X/774/2/99 , https://ui.adsabs.harvard.edu/abs/2013ApJ...774...99K 774, 99
-
[45]
E., Childress M., Scharw \"a chter J., Do T., Schmidt B
Kerzendorf W. E., Childress M., Scharw \"a chter J., Do T., Schmidt B. P., 2014, @doi [ ] 10.1088/0004-637X/782/1/27 , https://ui.adsabs.harvard.edu/abs/2014ApJ...782...27K 782, 27
-
[46]
Kerzendorf W. E., Strampelli G., Shen K. J., Schwab J., Pakmor R., Do T., Buchner J., Rest A., 2018, @doi [ ] 10.1093/mnras/sty1357 , https://ui.adsabs.harvard.edu/abs/2018MNRAS.479..192K 479, 192
-
[47]
Kleinman S. J., et al., 2013, @doi [ ] 10.1088/0067-0049/204/1/5 , https://ui.adsabs.harvard.edu/abs/2013ApJS..204....5K 204, 5
-
[48]
Koester D., 2010, Memorie della Societa Astronomica Italiana, https://ui.adsabs.harvard.edu/abs/2010MmSAI..81..921K 81, 921
2010
-
[49]
Koposov S. E., et al., 2020, @doi [ ] 10.1093/mnras/stz3081 , https://ui.adsabs.harvard.edu/abs/2020MNRAS.491.2465K 491, 2465
-
[50]
L., 1993, ATLAS9 Stellar Atmosphere Programs and 2 km/s grid , Kurucz CD-ROM No
Kurucz R. L., 1993, ATLAS9 Stellar Atmosphere Programs and 2 km/s grid , Kurucz CD-ROM No. 13
1993
-
[51]
Leonard P. J. T., 1991, @doi [ ] 10.1086/115704 , https://ui.adsabs.harvard.edu/abs/1991AJ....101..562L 101, 562
-
[52]
Li W., Chornock R., Leaman J., Filippenko A. V., Poznanski D., Wang X., Ganeshalingam M., Mannucci F., 2011, @doi [ ] 10.1111/j.1365-2966.2011.18162.x , https://ui.adsabs.harvard.edu/abs/2011MNRAS.412.1473L 412, 1473
-
[53]
Lindegren L., 2018, R e-normalising the astrometric chi-square in G aia D R 2, GAIA-C3-TN-LU-LL-124, https://dms.cosmos.esa.int/COSMOS/doc_fetch.php?id=3757412
2018
-
[54]
Lindegren L., et al., 2021, @doi [ ] 10.1051/0004-6361/202039709 , https://ui.adsabs.harvard.edu/abs/2021A&A...649A...2L 649, A2
-
[55]
Mackensen N., Reindl N., Werner K., Dorsch M., Tan S., 2025, @doi [ ] 10.1051/0004-6361/202554639 , https://ui.adsabs.harvard.edu/abs/2025A&A...700A..24M 700, A24
-
[56]
S., Fremling, C., & Kasliwal, M
Mandigo-Stoba M. S., Fremling C., Kasliwal M. M., 2022, @doi [Journal of Open Source Software] 10.21105/joss.03612 , 7, 3612
-
[57]
Maoz D., Mannucci F., Brandt T. D., 2012, @doi [ ] 10.1111/j.1365-2966.2012.21871.x , https://ui.adsabs.harvard.edu/abs/2012MNRAS.426.3282M 426, 3282
-
[58]
Maoz D., Mannucci F., Nelemans G., 2014, @doi [ ] 10.1146/annurev-astro-082812-141031 , https://ui.adsabs.harvard.edu/abs/2014ARA&A..52..107M 52, 107
-
[59]
Marietta E., Burrows A., Fryxell B., 2000, @doi [ ] 10.1086/313392 , https://ui.adsabs.harvard.edu/abs/2000ApJS..128..615M 128, 615
-
[60]
Marshall J. L., et al., 2008, in McLean I. S., Casali M. M., eds, Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series Vol. 7014, Ground-based and Airborne Instrumentation for Astronomy II. p. 701454 ( @eprint arXiv 0807.3774 ), @doi 10.1117/12.789972
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1117/12.789972 2008
-
[61]
Mehta V., Tiwari V., Pakmor R., Singh D., Fisher R., 2026, arXiv e-prints, https://ui.adsabs.harvard.edu/abs/2026arXiv260223414M p. arXiv:2602.23414
-
[62]
Nagarajan P., El-Badry K., Rodriguez A. C., van Roestel J., Roulston B., 2023, @doi [arXiv e-prints] 10.48550/arXiv.2304.07324 , https://ui.adsabs.harvard.edu/abs/2023arXiv230407324N p. arXiv:2304.07324
-
[63]
Neunteufel P., 2020, @doi [ ] 10.1051/0004-6361/202037792 , https://ui.adsabs.harvard.edu/abs/2020A&A...641A..52N 641, A52
-
[64]
Neunteufel P., Preece H., Kruckow M., Geier S., Hamers A. S., Justham S., Podsiadlowski P., 2022, @doi [ ] 10.1051/0004-6361/202142864 , https://ui.adsabs.harvard.edu/abs/2022A&A...663A..91N 663, A91
-
[65]
Nottale L., Chamaraux P., 2018, @doi [ ] 10.1051/0004-6361/201832707 , https://ui.adsabs.harvard.edu/abs/2018A&A...614A..45N 614, A45
-
[66]
Oke J. B., Gunn J. E., 1982, @doi [ ] 10.1086/131027 , https://ui.adsabs.harvard.edu/abs/1982PASP...94..586O 94, 586
-
[67]
Oke J. B., et al., 1995, @doi [ ] 10.1086/133562 , https://ui.adsabs.harvard.edu/abs/1995PASP..107..375O 107, 375
-
[68]
Pakmor R., et al., 2022, @doi [ ] 10.1093/mnras/stac3107 , https://ui.adsabs.harvard.edu/abs/2022MNRAS.517.5260P 517, 5260
-
[69]
Pakmor R., et al., 2025, @doi [arXiv e-prints] 10.48550/arXiv.2510.11781 , https://ui.adsabs.harvard.edu/abs/2025arXiv251011781P p. arXiv:2510.11781
-
[70]
Pan K.-C., Ricker P. M., Taam R. E., 2012, @doi [ ] 10.1088/0004-637X/760/1/21 , https://ui.adsabs.harvard.edu/abs/2012ApJ...760...21P 760, 21
-
[71]
Paxton B., Bildsten L., Dotter A., Herwig F., Lesaffre P., Timmes F., 2011, @doi [ ] 10.1088/0067-0049/192/1/3 , https://ui.adsabs.harvard.edu/abs/2011ApJS..192....3P 192, 3
-
[72]
Paxton B., et al., 2013, @doi [ ] 10.1088/0067-0049/208/1/4 , https://ui.adsabs.harvard.edu/abs/2013ApJS..208....4P 208, 4
work page internal anchor Pith review doi:10.1088/0067-0049/208/1/4 2013
-
[73]
Paxton B., et al., 2015, @doi [ ] 10.1088/0067-0049/220/1/15 , https://ui.adsabs.harvard.edu/abs/2015ApJS..220...15P 220, 15
work page internal anchor Pith review doi:10.1088/0067-0049/220/1/15 2015
-
[74]
Paxton B., et al., 2018, @doi [ ] 10.3847/1538-4365/aaa5a8 , https://ui.adsabs.harvard.edu/abs/2018ApJS..234...34P 234, 34
work page internal anchor Pith review doi:10.3847/1538-4365/aaa5a8 2018
-
[75]
Paxton B., et al., 2019, @doi [ ] 10.3847/1538-4365/ab2241 , https://ui.adsabs.harvard.edu/abs/2019ApJS..243...10P 243, 10
-
[76]
Perley D. A., 2019, @doi [ ] 10.1088/1538-3873/ab215d , https://ui.adsabs.harvard.edu/abs/2019PASP..131h4503P 131, 084503
-
[77]
Pollin J. M., Sim S. A., Pakmor R., Callan F. P., Collins C. E., Shingles L. J., R \"o pke F. K., Srivastav S., 2024, @doi [ ] 10.1093/mnras/stae1909 , https://ui.adsabs.harvard.edu/abs/2024MNRAS.533.3036P 533, 3036
-
[78]
Prochaska J. X., Hennawi J. F., Westfall K. B., Cooke R. J., Wang F., Hsyu T., Davies F. B., Farina E. P., 2020, arXiv e-prints, https://ui.adsabs.harvard.edu/abs/2020arXiv200506505P p. arXiv:2005.06505
-
[79]
Prust L. J., Bildsten L., Boos S. J., 2026, @doi [ ] 10.3847/1538-4357/ae22db , https://ui.adsabs.harvard.edu/abs/2026ApJ...997...17P 997, 17
-
[80]
Raddi R., et al., 2019, @doi [ ] 10.1093/mnras/stz1618 , https://ui.adsabs.harvard.edu/abs/2019MNRAS.489.1489R 489, 1489
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.