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arxiv: 2605.05308 · v1 · submitted 2026-05-06 · 🌌 astro-ph.SR · astro-ph.HE

Recognition: unknown

The diverse outcomes of binary white dwarf mergers and connections to Galactic LISA sources

Claire S. Ye, Katelyn Breivik, Kyle Kremer

Authors on Pith no claims yet

Pith reviewed 2026-05-08 15:33 UTC · model grok-4.3

classification 🌌 astro-ph.SR astro-ph.HE
keywords white dwarf binariesmerger outcomespopulation synthesisLISAgravitational wavesMilky Waybinary evolutionType Ia supernovae
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The pith

Public mock catalogs of Milky Way white dwarf mergers connect LISA gravitational wave data to specific binary evolution outcomes.

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

The authors generate suites of mock catalogs for the Milky Way's white dwarf merger history with the COSMIC population synthesis code. These catalogs track how white dwarf masses and chemical compositions determine merger results such as AM CVn binaries, R Coronae Borealis stars, young rapidly spinning white dwarfs, magnetars, and Type Ia supernovae. The work maps how rates of each outcome shift when binary evolution assumptions, including mass transfer stability and common-envelope ejection, are varied. Public release of the catalogs supplies a direct tool for matching LISA-detected close white dwarf binaries to their long-term electromagnetic fates.

Core claim

Using the COSMIC population synthesis code, the authors create suites of mock catalogs representing the white dwarf merger history of the Milky Way. These catalogs summarize expected merger outcomes based on white dwarf masses and compositions and show how rates vary with binary evolution model uncertainties. The catalogs are released publicly to enable connections between LISA gravitational wave science and white dwarf binary astrophysics.

What carries the argument

The COSMIC population synthesis code, which evolves binary systems from initial masses and separations through mass transfer and common-envelope phases to produce predicted merger outcomes and their rates.

If this is right

  • Different white dwarf masses and compositions produce distinct merger products ranging from stable mass-transferring systems to explosive transients.
  • Uncertainties in binary evolution parameters change the relative rates of these outcomes across the Galaxy.
  • LISA observations of close white dwarf binaries can be cross-matched with the catalogs to forecast their future electromagnetic signatures.
  • The public catalogs enable combined gravitational-wave and electromagnetic studies of white dwarf binary populations.

Where Pith is reading between the lines

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

  • Updated catalogs incorporating tighter constraints on common-envelope efficiency could narrow the allowed range of merger rates for each outcome class.
  • The same simulation framework could be extended to predict LISA source counts for other compact-object binaries such as neutron star pairs.
  • Direct counting of observed merger products in the Milky Way would provide an independent check on the binary evolution physics assumed in the models.

Load-bearing premise

The COSMIC code accurately models the uncertain physics of binary white dwarf evolution including mass transfer stability and common-envelope ejection.

What would settle it

A mismatch between the fraction of LISA-detected white dwarf binaries that evolve into each predicted outcome class, such as Type Ia supernovae versus stable AM CVn systems, and the distributions in the released catalogs when the same binaries are followed forward.

Figures

Figures reproduced from arXiv: 2605.05308 by Claire S. Ye, Katelyn Breivik, Kyle Kremer.

Figure 1
Figure 1. Figure 1: Summary of outcomes of white dwarf mergers for various component masses, M1 and M2. The solid black lines denote the approximate boundaries between different white dwarf compositions: He (< 0.5 M⊙), CO (0.5 − 1.1 M⊙), and O/Ne (> 1.1 M⊙). The diagonal solid line denotes the Chandrasekhar limit : M1 + M2 = 1.4 M⊙. The two dashed curves mark the boundaries between disk and direct impact accretion (bottom cur… view at source ↗
Figure 2
Figure 2. Figure 2: Secondary (M2) versus primary (M1) masses for all white dwarf mergers occurring throughout the full history of each of our Galactic population models. We mark the same six regions indicated in view at source ↗
Figure 3
Figure 3. Figure 3: Same as view at source ↗
Figure 4
Figure 4. Figure 4: Delay time distributions (time from star formation to Roche contact) for all white dwarf pair combinations (columns from left to right) and Galactic model assumptions (rows from top to bottom). For each panel, we separate all white dwarf mergers into five metallicity bins centered on [Fe/H] =[-2.05, -1.56, -1.06, -0.56, -0.07]. cial and q3 models. In the α = 5 variation, the second phase of mass transfer d… view at source ↗
Figure 5
Figure 5. Figure 5: Colored curves show merger time distributions (in units of absolute Cosmic time) for all white dwarf pair combinations (columns) and binary evolution assumptions (rows). The solid gray histogram in each panel shows the distribution of star formation times for each white dwarf merger. In the insets, we zoom in on the most recent 100 Myr of Galactic history. Colored curves in the insets show the number of me… view at source ↗
Figure 6
Figure 6. Figure 6: Same as view at source ↗
read the original abstract

In the coming decade, the millihertz gravitational wave observatory LISA will provide the best constraints yet on the tens of thousands of close white dwarf binaries in the Milky Way, yielding unprecedented insights into the most abundant class of compact object binaries. Following inspiral via gravitational wave emission, interacting white dwarf binary pairs can lead to a multitude of outcomes, including AM Canum Venaticorum (AM CVn) binaries, R Coronae Borealis stars, young, rapidly-spinning single white dwarfs, (millisecond) magnetars, and a variety of explosive transients, most notably Type Ia supernovae. Current and future electromagnetic observations of these various outcomes coupled with the forthcoming flood of data from LISA place us on the precipice of a significant advance in our understanding of the long-term fate of white dwarf binaries. In this paper, we present a suite of mock catalogs of the Milky Way's white dwarf merger history, created using the population synthesis code $\texttt{COSMIC}$. We summarize the various merger outcomes expected (based upon varying white dwarf masses and chemical compositions) and explore ways the rates of these outcomes may vary with model uncertainties pertaining to binary evolution. We publicly release these merger catalogs as a tool for facilitating connections between gravitational wave science and white dwarf binary astrophysics.

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 / 2 minor

Summary. The paper uses the COSMIC population synthesis code to generate a suite of mock catalogs of Milky Way white dwarf binary merger histories. It summarizes expected merger outcomes (AM CVn binaries, RCB stars, magnetars, SNe Ia and other transients) as a function of white dwarf masses and compositions, explores variations in outcome rates arising from uncertainties in binary evolution parameters, and publicly releases the catalogs to support connections between LISA gravitational-wave observations and white dwarf astrophysics.

Significance. If the underlying COSMIC modeling is reliable, the public catalogs would provide a practical resource for linking future LISA detections of close white dwarf binaries to their electromagnetic outcomes and for testing binary evolution models. The forward-modeling approach and explicit release of the catalogs are clear strengths. However, the absence of any quantitative validation, error budgets, or comparisons to observed populations substantially limits the immediate scientific impact.

major comments (2)
  1. [Section 3] Section 3 (Merger Outcomes): the manuscript presents predicted fractions and rates for each outcome class but supplies no comparison to observed rates (e.g., Galactic SN Ia rate, AM CVn space density, or RCB star counts) or to results from independent population-synthesis codes; this omission is load-bearing for the claim that the catalogs are ready tools for LISA science.
  2. [Section 4] Section 4 (Model Uncertainties): while common-envelope efficiency and a few other parameters are varied, the paper does not document or test the specific COSMIC prescriptions for mass-transfer stability, common-envelope ejection, and the progenitor-to-WD composition mapping that determine the final merger products; without such tests the explored variations cannot be shown to bracket the true uncertainty.
minor comments (2)
  1. [Abstract] The abstract states that catalogs are released but does not specify the total number of realizations, the exact parameter grid, or the data format; adding these details would improve usability.
  2. [Figures] Figure captions and axis labels in the results figures should explicitly state which binary-evolution parameters are held fixed versus varied in each panel.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their constructive and detailed report. We agree that strengthening the documentation of COSMIC prescriptions and providing context for the model predictions relative to observations will improve the manuscript's utility. We respond point-by-point to the major comments below and indicate the revisions we will make.

read point-by-point responses
  1. Referee: [Section 3] Section 3 (Merger Outcomes): the manuscript presents predicted fractions and rates for each outcome class but supplies no comparison to observed rates (e.g., Galactic SN Ia rate, AM CVn space density, or RCB star counts) or to results from independent population-synthesis codes; this omission is load-bearing for the claim that the catalogs are ready tools for LISA science.

    Authors: We acknowledge that explicit comparisons would help users assess the catalogs for LISA applications. The core purpose of the paper is to generate and publicly release the COSMIC mock catalogs so that the community can perform tailored comparisons incorporating selection effects and specific science cases. To address the concern, we will revise Section 3 to include a short discussion referencing literature values for key rates (e.g., the Milky Way SN Ia rate of approximately 0.003 yr^{-1} and AM CVn space densities from observational surveys) and note that our predicted outcome fractions lie within the broad ranges reported in the literature and other population synthesis studies. We will add a clear caveat that full quantitative validation requires modeling of observational biases and is facilitated by the released catalogs rather than performed here. This addition will support the utility claim without overstepping the paper's scope. revision: partial

  2. Referee: [Section 4] Section 4 (Model Uncertainties): while common-envelope efficiency and a few other parameters are varied, the paper does not document or test the specific COSMIC prescriptions for mass-transfer stability, common-envelope ejection, and the progenitor-to-WD composition mapping that determine the final merger products; without such tests the explored variations cannot be shown to bracket the true uncertainty.

    Authors: We agree that more explicit documentation of the underlying prescriptions is needed. The mass-transfer stability criterion (based on the adiabatic response of the donor star), common-envelope ejection (alpha-lambda formalism with lambda from stellar structure), and progenitor-to-WD composition mapping (using SSE/BSE evolutionary tracks for initial mass and metallicity) are fully specified in the COSMIC reference paper (Breivik et al. 2020). We will add a dedicated subsection to Section 4 that summarizes these prescriptions, including the default parameter choices and equations used in our simulations, with direct references to the COSMIC documentation. We will also clarify that the parameter variations (including common-envelope efficiency) are intended to illustrate sensitivity to major uncertainties rather than to exhaustively bracket every possible variation in binary evolution physics. This revision will make the explored range more transparent without requiring new simulations. revision: yes

Circularity Check

0 steps flagged

No circularity: forward population synthesis from external code inputs

full rationale

The paper performs forward modeling of Milky Way white dwarf merger catalogs using the established COSMIC population synthesis code, varying binary evolution parameters (common-envelope efficiency, mass-transfer stability) to explore outcome distributions (AM CVn, RCB, SNe Ia, etc.). No equations, fitted parameters, or self-referential definitions are present that reduce claimed outputs back to inputs by construction. The catalogs are direct simulation products; model uncertainties are propagated explicitly rather than fitted to match targets. Self-citation to COSMIC (if present) is tool usage, not load-bearing justification of a derived result. The derivation chain is self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central results rest on the COSMIC code's internal modeling of binary evolution, which incorporates numerous uncertain parameters whose values are chosen rather than derived from first principles.

free parameters (1)
  • common-envelope efficiency and other binary-evolution parameters
    These parameters control merger rates and outcome branching ratios and are varied to explore model uncertainties as stated in the abstract.
axioms (1)
  • domain assumption Standard stellar and binary evolution prescriptions implemented in the COSMIC population synthesis code are sufficiently accurate for the mass and composition ranges considered.
    The abstract relies on these prescriptions to generate the mock catalogs without providing independent verification.

pith-pipeline@v0.9.0 · 5537 in / 1403 out tokens · 71685 ms · 2026-05-08T15:33:26.578021+00:00 · methodology

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Works this paper leans on

141 extracted references · 138 canonical work pages · 1 internal anchor

  1. [1]

    Living Rev

    Amaro-Seoane, P., Andrews, J., Arca Sedda, M., et al. 2023, Living Reviews in Relativity, 26, 2, doi: 10.1007/s41114-022-00041-y

  2. [2]

    2014, MNRAS, 439, 1079, doi: 10.1093/mnras/stu039

    Amaro-Seoane, P. 2014, MNRAS, 439, 1079, doi: 10.1093/mnras/stu039

  3. [3]

    Gladstone, J. C. 2013, ApJ, 766, 136, doi: 10.1088/0004-637X/766/2/136

  4. [4]

    Belczynski, K., Bulik, T., & Ruiter, A. J. 2005, ApJ, 629, 915, doi: 10.1086/431578

  5. [5]

    A., et al

    Belczynski, K., Kalogera, V., Rasio, F. A., et al. 2008, ApJS, 174, 223, doi: 10.1086/521026 16

  6. [6]

    I - 0.9 and 1.2 solar mass stars

    Benz, W., Bowers, R. L., Cameron, A. G. W., & Press, W. H. . 1990, ApJ, 348, 647, doi: 10.1086/168273

  7. [7]

    J., Weinberg, N

    Bildsten, L., Shen, K. J., Weinberg, N. N., & Nelemans, G. 2007, ApJL, 662, L95, doi: 10.1086/519489

  8. [8]

    N., Gnedin, O

    Bregman, J. N., Gnedin, O. Y., Seitzer, P. O., & Qu, Z. 2024, ApJL, 968, L6, doi: 10.3847/2041-8213/ad498f

  9. [9]

    2018, ApJL, 854, L1, doi: 10.3847/2041-8213/aaaa23

    Breivik, K., Kremer, K., Bueno, M., et al. 2018, ApJL, 854, L1, doi: 10.3847/2041-8213/aaaa23

  10. [10]

    Breivik, K., Mingarelli, C. M. F., & Larson, S. L. 2020a, ApJ, 901, 4, doi: 10.3847/1538-4357/abab99

  11. [11]

    2020 , note =

    Breivik, K., Coughlin, S., Zevin, M., et al. 2020b, ApJ, 898, 71, doi: 10.3847/1538-4357/ab9d85

  12. [12]

    2017, ApJ, 850, 127, doi: 10.3847/1538-4357/aa9568

    Brooks, J., Schwab, J., Bildsten, L., et al. 2017, ApJ, 850, 127, doi: 10.3847/1538-4357/aa9568

  13. [13]

    P., Ferrario, L., Pakmor, R., et al

    Burmester, U. P., Ferrario, L., Pakmor, R., et al. 2023, MNRAS, 523, 527, doi: 10.1093/mnras/stad1394

  14. [14]

    B., Fuller, J., et al

    Caiazzo, I., Burdge, K. B., Fuller, J., et al. 2021, Nature, 595, 39, doi: 10.1038/s41586-021-03615-y

  15. [15]

    B., Tremblay, P.-E., et al

    Caiazzo, I., Burdge, K. B., Tremblay, P.-E., et al. 2023, Nature, 620, 61, doi: 10.1038/s41586-023-06171-9

  16. [16]

    2014, A&A, 566, A86, doi: 10.1051/0004-6361/201323052

    Camacho, J., Torres, S., Garc´ ıa-Berro, E., et al. 2014, A&A, 566, A86, doi: 10.1051/0004-6361/201323052

  17. [17]

    J., Marsh, T

    Carter, P. J., Marsh, T. R., Steeghs, D., et al. 2013, MNRAS, 429, 2143, doi: 10.1093/mnras/sts485

  18. [18]

    D., & M´ enard, B

    Cheng, S., Cummings, J. D., & M´ enard, B. 2019, ApJ, 886, 100, doi: 10.3847/1538-4357/ab4989

  19. [19]

    D., M´ enard, B., & Toonen, S

    Cheng, S., Cummings, J. D., M´ enard, B., & Toonen, S. 2020, ApJ, 891, 160, doi: 10.3847/1538-4357/ab733c

  20. [20]

    Verbunt, F. W. M. 2014, A&A, 563, A83, doi: 10.1051/0004-6361/201322714

  21. [21]

    Clark, G. W. 1975, ApJL, 199, L143, doi: 10.1086/181869

  22. [22]

    Clayton, G. C. 1996, PASP, 108, 225, doi: 10.1086/133715

  23. [23]

    2007, ApJ, 662, 1220, doi: 10.1086/518307

    Asplund, M. 2007, ApJ, 662, 1220, doi: 10.1086/518307

  24. [24]

    M., Piotto, G., & King, I

    Cool, A. M., Piotto, G., & King, I. R. 1996, ApJ, 468, 655, doi: 10.1086/177723

  25. [25]

    2019, ApJ, 885, 74, doi: 10.3847/1538-4357/ab46b9 de Wit, J., Alonso, R., Rackham, B

    Coutu, S., Dufour, P., Bergeron, P., et al. 2019, ApJ, 885, 74, doi: 10.3847/1538-4357/ab46b9

  26. [26]

    2014, MNRAS, 438, 14, doi: 10.1093/mnras/stt1766

    Dan, M., Rosswog, S., Br¨ uggen, M., & Podsiadlowski, P. 2014, MNRAS, 438, 14, doi: 10.1093/mnras/stt1766

  27. [27]

    2011, ApJ, 737, 89, doi: 10.1088/0004-637X/737/2/89 De Marco, O

    Dan, M., Rosswog, S., Guillochon, J., & Ramirez-Ruiz, E. 2011, ApJ, 737, 89, doi: 10.1088/0004-637X/737/2/89 De Marco, O. 2009, PASP, 121, 316, doi: 10.1086/597765

  28. [28]

    D., et al

    Dessart, L., Burrows, A., Ott, C. D., et al. 2006, ApJ, 644, 1063, doi: 10.1086/503626

  29. [29]

    R., Chornock, R., Soderberg, A

    Drout, M. R., Chornock, R., Soderberg, A. M., et al. 2014, ApJ, 794, 23, doi: 10.1088/0004-637X/794/1/23

  30. [30]

    H., & Clemens, J

    Dunlap, B. H., & Clemens, J. C. 2015, in Astronomical Society of the Pacific Conference Series, Vol. 493, 19th European Workshop on White Dwarfs, ed. P. Dufour, P. Bergeron, & G. Fontaine, 547

  31. [31]

    A., & Hirata, C

    Fang, X., Thompson, T. A., & Hirata, C. M. 2018, MNRAS, 476, 4234, doi: 10.1093/mnras/sty472

  32. [32]

    Ferrario, L., de Martino, D., & G¨ ansicke, B. T. 2015, SSRv, 191, 111, doi: 10.1007/s11214-015-0152-0

  33. [33]

    K., Hillebrandt, W., et al

    Fink, M., R¨ opke, F. K., Hillebrandt, W., et al. 2010, A&A, 514, A53, doi: 10.1051/0004-6361/200913892

  34. [34]

    Rasio, F. A. 2019, ApJ, 872, 165, doi: 10.3847/1538-4357/ab0214

  35. [35]

    M., & Frank, J

    Gokhale, V., Peng, X. M., & Frank, J. 2007, ApJ, 655, 1010, doi: 10.1086/510119

  36. [36]

    J., van Roestel, J., & Wong, T

    Green, M. J., van Roestel, J., & Wong, T. L. S. 2025, A&A, 700, A107, doi: 10.1051/0004-6361/202554925

  37. [37]

    2004, A&A, 413, 257, doi: 10.1051/0004-6361:20031504

    Guerrero, J., Garc´ ıa-Berro, E., & Isern, J. 2004, A&A, 413, 257, doi: 10.1051/0004-6361:20031504

  38. [38]

    2010, ApJL, 709, L64, doi: 10.1088/2041-8205/709/1/L64

    Guillochon, J., Dan, M., Ramirez-Ruiz, E., & Rosswog, S. 2010, ApJL, 709, L64, doi: 10.1088/2041-8205/709/1/L64

  39. [39]

    V., Gr¨ afener, G., Langer, N., et al

    Gvaramadze, V. V., Gr¨ afener, G., Langer, N., et al. 2019, Nature, 569, 684, doi: 10.1038/s41586-019-1216-1

  40. [40]

    Han, Z., Podsiadlowski, P., & Eggleton, P. P. 1995, MNRAS, 272, 800, doi: 10.1093/mnras/272.4.800

  41. [41]

    Han, Z., Podsiadlowski, P., Maxted, P. F. L., & Marsh, T. R. 2003, MNRAS, 341, 669, doi: 10.1046/j.1365-8711.2003.06451.x

  42. [42]

    Hansen, B. M. S., Kalirai, J. S., Anderson, J., et al. 2013, Nature, 500, 51, doi: 10.1038/nature12334

  43. [43]

    2025, ApJ, 986, 123, doi: 10.3847/1538-4357/add32b

    He, W., Zhou, P., Gjergo, E., & Fu, X. 2025, ApJ, 986, 123, doi: 10.3847/1538-4357/add32b

  44. [44]

    2016, PASP, 128, 082001, doi: 10.1088/1538-3873/128/966/082001

    Heber, U. 2016, PASP, 128, 082001, doi: 10.1088/1538-3873/128/966/082001

  45. [45]

    FIRE-2 Simulations: Physics versus Numerics in Galaxy Formation

    Hopkins, P. F., Wetzel, A., Kereˇ s, D., et al. 2018, MNRAS, 480, 800, doi: 10.1093/mnras/sty1690

  46. [46]

    R., Tout, C

    Hurley, J. R., Tout, C. A., & Pols, O. R. 2002, MNRAS, 329, 897, doi: 10.1046/j.1365-8711.2002.05038.x

  47. [47]

    1990, ApJ, 353, 215, doi: 10.1086/168609

    Iben, Jr., I. 1990, ApJ, 353, 215, doi: 10.1086/168609

  48. [48]

    Iben, Jr., I., & Tutukov, A. V. 1984, ApJS, 54, 335, doi: 10.1086/190932 —. 1985, ApJS, 58, 661, doi: 10.1086/191054 —. 1987, ApJ, 313, 727, doi: 10.1086/165011

  49. [49]

    V., & Yungelson, L

    Iben, Jr., I., Tutukov, A. V., & Yungelson, L. R. 1997, ApJ, 475, 291, doi: 10.1086/303525

  50. [50]

    J., Lucas, P

    Justham, S., Podsiadlowski, P., & Han, Z. 2011, MNRAS, 410, 984, doi: 10.1111/j.1365-2966.2010.17497.x

  51. [51]

    Katz, J. I. 1975, Nature, 253, 698, doi: 10.1038/253698a0

  52. [52]

    J., Gianninas, A., et al

    Kilic, M., Hermes, J. J., Gianninas, A., et al. 2014, MNRAS, 438, L26, doi: 10.1093/mnrasl/slt151 17

  53. [53]

    R., Pringle, J

    King, A. R., Pringle, J. E., & Wickramasinghe, D. T. 2001, MNRAS, 320, L45, doi: 10.1046/j.1365-8711.2001.04184.x

  54. [54]

    2022, Nature, 602, 585, doi: 10.1038/s41586-021-04354-w

    Kirsten, F., Marcote, B., Nimmo, K., et al. 2022, Nature, 602, 585, doi: 10.1038/s41586-021-04354-w

  55. [55]

    S., Janka, H.-T., & Hillebrandt, W

    Kitaura, F. S., Janka, H.-T., & Hillebrandt, W. 2006, A&A, 450, 345, doi: 10.1051/0004-6361:20054703

  56. [56]

    Koester, D., & Kepler, S. O. 2019, A&A, 628, A102, doi: 10.1051/0004-6361/201935946

  57. [57]

    2022, MNRAS, 511, 5936, doi:10.1093/mnras/stac415 Kovács, O

    Korol, V., Hallakoun, N., Toonen, S., & Karnesis, N. 2022, MNRAS, 511, 5936, doi: 10.1093/mnras/stac415

  58. [58]

    M., Groot, P

    Korol, V., Rossi, E. M., Groot, P. J., et al. 2017, MNRAS, 470, 1894, doi: 10.1093/mnras/stx1285

  59. [59]

    , year = 1962, month = nov, volume =

    Kozai, Y. 1962, AJ, 67, 591, doi: 10.1086/108790

  60. [60]

    2026, in Encyclopedia of Astrophysics, Volume 3, Vol

    Kremer, K. 2026, in Encyclopedia of Astrophysics, Volume 3, Vol. 3, 458–472, doi: 10.1016/B978-0-443-21439-4.00103-6

  61. [61]

    L., & Kalogera, V

    Kremer, K., Breivik, K., Larson, S. L., & Kalogera, V. 2017, ApJ, 846, 95, doi: 10.3847/1538-4357/aa8557

  62. [62]

    L., & Ransom, S

    Kremer, K., Fuller, J., Piro, A. L., & Ransom, S. M. 2023, MNRAS, 525, L22, doi: 10.1093/mnrasl/slad088

  63. [63]

    L., & Li, D

    Kremer, K., Piro, A. L., & Li, D. 2021a, ApJL, 917, L11, doi: 10.3847/2041-8213/ac13a0

  64. [64]

    Z., Weatherford, N

    Kremer, K., Rui, N. Z., Weatherford, N. C., et al. 2021b, ApJ, 917, 28, doi: 10.3847/1538-4357/ac06d4

  65. [65]

    2015, ApJ, 806, 76, doi: 10.1088/0004-637X/806/1/76

    Kremer, K., Sepinsky, J., & Kalogera, V. 2015, ApJ, 806, 76, doi: 10.1088/0004-637X/806/1/76

  66. [66]

    2001, MNRAS, 322, 231

    Kroupa, P. 2001, MNRAS, 322, 231

  67. [67]

    B., et al

    Lamberts, A., Blunt, S., Littenberg, T. B., et al. 2019, MNRAS, 490, 5888, doi: 10.1093/mnras/stz2834

  68. [68]

    2011, MNRAS, 418, 467, doi: 10.1111/j.1365-2966.2011.19497.x

    Li, W., Chornock, R., Leaman, J., et al. 2011, MNRAS, 412, 1473, doi: 10.1111/j.1365-2966.2011.18162.x

  69. [69]

    Lidov, M. L. 1962, Planet. Space Sci., 9, 719, doi: 10.1016/0032-0633(62)90129-0

  70. [70]

    M., & Postnov, K

    Lipunov, V. M., & Postnov, K. A. 1988, Ap&SS, 145, 1, doi: 10.1007/BF00645692

  71. [71]

    Research in Astronomy and Astrophysics , keywords =

    Liu, Z.-W., R¨ opke, F. K., & Han, Z. 2023, Research in Astronomy and Astrophysics, 23, 082001, doi: 10.1088/1674-4527/acd89e

  72. [72]

    1990, ApJL, 354, L53, doi: 10.1086/185721 Lor´ en-Aguilar, P., Isern, J., & Garc´ ıa-Berro, E

    Livne, E. 1990, ApJL, 354, L53, doi: 10.1086/185721 Lor´ en-Aguilar, P., Isern, J., & Garc´ ıa-Berro, E. 2009, A&A, 500, 1193, doi: 10.1051/0004-6361/200811060

  73. [73]

    Lorimer, D. R. 2008, Living Reviews in Relativity, 11, 8, doi: 10.12942/lrr-2008-8

  74. [74]

    2022, MNRAS, 510, 1867, doi: 10.1093/mnras/stab3500

    Lu, W., Beniamini, P., & Kumar, P. 2022, MNRAS, 510, 1867, doi: 10.1093/mnras/stab3500

  75. [75]

    2012, PASA, 29, 447, doi: 10.1071/AS11052

    Maoz, D., & Mannucci, F. 2012, PASA, 29, 447, doi: 10.1071/AS11052

  76. [76]

    2014, ARA&A, 52, 107, https://doi.org/10.1146/annurev-astro-082812-141031

    Maoz, D., Mannucci, F., & Nelemans, G. 2014, ARA&A, 52, 107, doi: 10.1146/annurev-astro-082812-141031

  77. [77]

    R., Nelemans, G., & Steeghs, D

    Marsh, T. R., Nelemans, G., & Steeghs, D. 2004, MNRAS, 350, 113, doi: 10.1111/j.1365-2966.2004.07564.x

  78. [78]

    2021, ApJ, 923, 100, doi: 10.3847/1538-4357/ac2a39

    Strader, J. 2021, ApJ, 923, 100, doi: 10.3847/1538-4357/ac2a39

  79. [79]

    1980, PASJ, 32, 303, doi: 10.1093/pasj/32.2.303

    Miyaji, S., Nomoto, K., Yokoi, K., & Sugimoto, D. 1980, PASJ, 32, 303, doi: 10.1093/pasj/32.2.303

  80. [80]

Showing first 80 references.