Where are Gaia's small black holes?
Pith reviewed 2026-05-18 22:56 UTC · model grok-4.3
The pith
Natal kicks disrupt wide Gaia binaries more frequently than tight gravitational-wave progenitors, accounting for the relative dearth of 2.5-5 solar mass black holes.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The relative dearth of objects between 2.5 and 5 solar masses in Gaia wide binaries compared to LVK mergers arises because Gaia progenitor binaries are more susceptible to disruption by natal kicks received by low-mass black holes, owing to their typically lower companion masses and larger orbital separations.
What carries the argument
Binary survival probability against natal kicks, calculated as a function of kick velocity, orbital separation, and companion mass before the supernova.
If this is right
- The mass gap is more evident in wide binaries due to selective disruption of low-mass black hole systems.
- GW mergers preferentially sample binaries that survive stronger kicks.
- The natal kick velocity distribution can be constrained by matching the observed fractions in both populations.
- Low-mass black holes form with kicks that are sufficient to unbind wide but not tight binaries.
Where Pith is reading between the lines
- If the explanation holds, the true black hole mass spectrum may not have a gap, with the observed gap being an observational selection effect.
- Similar kick biases could affect other surveys of wide binaries versus merging systems.
- Population synthesis models should incorporate these differential survival rates to predict detection rates.
- Direct measurement of black hole velocities in disrupted systems could test the kick strength required.
Load-bearing premise
Gaia and GW progenitor binaries have different pre-supernova companion masses and orbital separations, leading to different survival rates against the same natal kicks for low-mass black holes.
What would settle it
Detection of a comparable fraction of 2.5-5 solar mass black holes in Gaia wide binaries, with binary parameters inconsistent with higher survival probabilities, would challenge the natal kick explanation.
Figures
read the original abstract
Gaia has recently revealed a population of over 20 compact objects in wide astrometric binaries, while LIGO-Virgo-KAGRA (LVK) have observed around 100 compact object binaries as gravitational-wave (GW) mergers. Despite belonging to different systems, the compact objects discovered by both Gaia and the LVK follow a multimodal mass distribution, with a global maximum at neutron star (NS) masses ($\sim 1$-$2\,M_\odot$) and a secondary local maximum at black hole (BH) masses $\sim10\,M_\odot$. However, the relative dearth of objects, or ``mass gap," between these modes is more pronounced among the wide binaries observed by Gaia compared to the GW population, with $9^{+10}_{-6}\%$ of GW component masses falling between $2.5$--$5\,M_\odot$ compared to $\lesssim5\%$ of Gaia compact objects. We explore whether this discrepancy can be explained by the natal kicks received by low-mass BHs. GW progenitor binaries may be more likely to survive natal kicks, because the newborn BH has a more massive companion and/or is in a tighter binary than Gaia progenitor binaries. We compare the survival probabilities of Gaia and GW progenitor binaries as a function of natal kick strength and pre-supernova binary parameters, and map out the parameter space and kick strength required to disrupt the progenitor binaries leading to low-mass BHs in Gaia systems more frequently than those in GW systems.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims that the more pronounced mass gap (2.5-5 M⊙) in Gaia wide astrometric binaries (≲5%) versus LVK GW mergers (9+10−6%) can be explained by natal kicks disrupting Gaia progenitor binaries more frequently than GW progenitor binaries, owing to systematic differences in pre-SN companion mass and orbital separation that reduce survival probability for the former population.
Significance. If the proposed mechanism is shown to quantitatively reproduce the observed difference in mass-gap fractions after proper population weighting, the result would provide a standard binary-evolution explanation for the Gaia-LVK discrepancy and highlight the sensitivity of wide-binary survival to kick velocity and pre-SN architecture.
major comments (2)
- [Survival probability analysis] The survival-probability comparison (abstract and main text section on natal-kick survival) maps the parameter space where Gaia-like systems are more easily disrupted, but does not integrate the survival curves over the actual occurrence-rate distributions of companion mass and pre-SN separation drawn from binary population synthesis for wide versus close post-SN channels. Without this weighting the calculation shows a possible mechanism rather than demonstrating that the mechanism produces the reported 5 % versus 9 % difference.
- [Abstract, paragraph on survival probabilities] The central claim that Gaia progenitors experience systematically lower kick survival rests on the assumption that wide-binary progenitors have, on average, lower companion masses or wider separations than GW progenitors; this assumption is stated but not quantified with explicit pre-SN parameter distributions or occurrence rates from binary evolution models.
minor comments (2)
- [Figures] Figure captions and axis labels for survival-probability plots should explicitly distinguish Gaia-wide versus GW-tight progenitor tracks.
- [Introduction] The error bars on the LVK mass-gap fraction (9+10−6 %) should be referenced to the specific catalog or analysis used.
Simulated Author's Rebuttal
We thank the referee for their constructive and detailed comments on our manuscript. We address the major comments point by point below. We agree that further quantification using population synthesis distributions would strengthen the quantitative link to the observed mass-gap fractions and plan to incorporate these elements in the revision.
read point-by-point responses
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Referee: [Survival probability analysis] The survival-probability comparison (abstract and main text section on natal-kick survival) maps the parameter space where Gaia-like systems are more easily disrupted, but does not integrate the survival curves over the actual occurrence-rate distributions of companion mass and pre-SN separation drawn from binary population synthesis for wide versus close post-SN channels. Without this weighting the calculation shows a possible mechanism rather than demonstrating that the mechanism produces the reported 5 % versus 9 % difference.
Authors: We agree that integrating the survival probabilities over the actual occurrence-rate distributions from binary population synthesis is required to quantitatively demonstrate that the mechanism reproduces the reported difference in mass-gap fractions. In the revised manuscript we will convolve the survival probability surfaces with the distributions of companion mass and pre-SN orbital separation drawn from standard binary evolution models for the wide (Gaia) and close (GW) channels. This will yield the expected fraction of disrupted low-mass BH progenitors in each population, allowing a direct comparison to the observed 5% versus 9% values. revision: yes
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Referee: [Abstract, paragraph on survival probabilities] The central claim that Gaia progenitors experience systematically lower kick survival rests on the assumption that wide-binary progenitors have, on average, lower companion masses or wider separations than GW progenitors; this assumption is stated but not quantified with explicit pre-SN parameter distributions or occurrence rates from binary evolution models.
Authors: We acknowledge that the manuscript states the systematic differences in pre-SN architecture but does not present the explicit distributions or occurrence rates. In the revision we will add a new subsection and accompanying figure that displays the pre-SN companion-mass and separation distributions obtained from binary population synthesis for wide astrometric binaries versus tight GW progenitors. We will report the mean values for each channel and show how these differences produce lower average survival probabilities for Gaia-like systems across the relevant range of kick velocities. revision: yes
Circularity Check
No significant circularity; explanation uses external models without data-fitting or self-referential reduction
full rationale
The paper's central derivation compares survival probabilities of Gaia versus GW progenitor binaries against natal kicks as a function of kick velocity and pre-supernova parameters (companion mass, orbital separation), mapping regions where Gaia-like systems are more easily disrupted. This is presented as a possible mechanism to explain the observed mass-gap difference (9% in GW vs ≲5% in Gaia). No equations or steps reduce the discrepancy to a fitted parameter drawn from the Gaia or LVK data itself, nor does the argument rely on a load-bearing self-citation whose uniqueness theorem or ansatz is imported without independent verification. The calculation remains self-contained against standard binary-evolution assumptions and external kick distributions.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Natal kicks are imparted to newborn black holes and affect binary survival depending on companion mass and orbital separation.
- domain assumption Gaia and LVK progenitor binaries have systematically different pre-supernova parameters.
Reference graph
Works this paper leans on
-
[1]
G., Abbott, R., Abouelfettouh, I., et al
Abac, A. G., Abbott, R., Abouelfettouh, I., et al. 2024, ApJL, 970, L34, doi: 10.3847/2041-8213/ad5beb
-
[2]
Physical Review Letters , archivePrefix = "arXiv", eprint =
Abbott, B. P., Abbott, R., Abbott, T. D., et al. 2016, PhRvL, 116, 061102, doi: 10.1103/PhysRevLett.116.061102 —. 2018, Living Reviews in Relativity, 21, 3, doi: 10.1007/s41114-018-0012-9 —. 2019, Physical Review X, 9, 031040, doi: 10.1103/PhysRevX.9.031040 —. 2020a, ApJL, 892, L3, doi: 10.3847/2041-8213/ab75f5
-
[3]
Abbott, R., Abbott, T. D., Abraham, S., et al. 2020b, ApJL, 896, L44, doi: 10.3847/2041-8213/ab960f —. 2021, Physical Review X, 11, 021053, doi: 10.1103/PhysRevX.11.021053
-
[4]
Abbott, R., Abbott, T. D., Acernese, F., et al. 2023a, Physical Review X, 13, 041039, doi: 10.1103/PhysRevX.13.041039 —. 2023b, Physical Review X, 13, 011048, doi: 10.1103/PhysRevX.13.011048
-
[5]
Acernese, F., Agathos, M., Agatsuma, K., et al. 2015, Classical and Quantum Gravity, 32, 024001, doi: 10.1088/0264-9381/32/2/024001
-
[6]
Eldridge, J. J., & Hurley, J. 2022, MNRAS, 512, 5717, doi: 10.1093/mnras/stac930
-
[7]
Akutsu, T., Ando, M., Arai, K., et al. 2021, Progress of Theoretical and Experimental Physics, 2021, 05A101, doi: 10.1093/ptep/ptaa125
-
[8]
2025, arXiv e-prints, arXiv:2505.23151, doi: 10.48550/arXiv.2505.23151
An, Q.-Y., Huang, Y., Gu, W.-M., et al. 2025, arXiv e-prints, arXiv:2505.23151, doi: 10.48550/arXiv.2505.23151
-
[9]
Andrews, J. J., & Kalogera, V. 2022, ApJ, 930, 159, doi: 10.3847/1538-4357/ac66d6
-
[10]
2024, arXiv e-prints, arXiv:2412.03461, doi: 10.48550/arXiv.2412.03461
Baibhav, V., & Kalogera, V. 2024, arXiv e-prints, arXiv:2412.03461, doi: 10.48550/arXiv.2412.03461
-
[11]
Orosz, J. A. 1998, ApJ, 499, 367, doi: 10.1086/305614
-
[12]
Kimball, C., & Andrews, J. J. 2023, ApJ, 959, 106, doi: 10.3847/1538-4357/ad0557
-
[13]
2023, MNRAS, 518, 5298, doi: 10.1093/mnras/stac3052
Biscoveanu, S., Landry, P., & Vitale, S. 2023, MNRAS, 518, 5298, doi: 10.1093/mnras/stac3052
-
[14]
Bolton, C. T. 1972, Nature Physical Science, 240, 124, doi: 10.1038/physci240124a0
-
[15]
1995, Monthly Notices of the Royal Astronomical Society, 274, 461, doi: 10.1093/mnras/274.2.461
Brandt, N., & Podsiadlowski, P. 1995, MNRAS, 274, 461, doi: 10.1093/mnras/274.2.461
-
[16]
Coleman, M. S. B. 2023, arXiv e-prints, arXiv:2311.12109, doi: 10.48550/arXiv.2311.12109
-
[17]
Callister, T. A., & Farr, W. M. 2024, Physical Review X, 14, 021005, doi: 10.1103/PhysRevX.14.021005
-
[18]
Callister, T. A., Farr, W. M., & Renzo, M. 2021, ApJ, 920, 157, doi: 10.3847/1538-4357/ac1347
-
[19]
Casares, J., & Jonker, P. G. 2014, SSRv, 183, 223, doi: 10.1007/s11214-013-0030-6
-
[20]
Chakrabarti, S., Simon, J. D., Craig, P. A., et al. 2023, AJ, 166, 6, doi: 10.3847/1538-3881/accf21
-
[21]
2022, ApJ, 931, 107, doi: 10.3847/1538-4357/ac60a5 Di Carlo, U
Chawla, C., Chatterjee, S., Breivik, K., et al. 2022, ApJ, 931, 107, doi: 10.3847/1538-4357/ac60a5 Di Carlo, U. N., Agrawal, P., Rodriguez, C. L., & Breivik, K. 2024, ApJ, 965, 22, doi: 10.3847/1538-4357/ad2f2c 17
-
[22]
2025, arXiv e-prints, arXiv:2505.22102, doi: 10.48550/arXiv.2505.22102
Disberg, P., & Mandel, I. 2025, arXiv e-prints, arXiv:2505.22102, doi: 10.48550/arXiv.2505.22102
-
[23]
2023, ApJ, 946, 16, doi: 10.3847/1538-4357/acb5ed
Edelman, B., Farr, B., & Doctor, Z. 2023, ApJ, 946, 16, doi: 10.3847/1538-4357/acb5ed
-
[24]
2024, New Astronomy Reviews, 98, 101694, doi: 10.1016/j.newar.2024.101694
El-Badry, K. 2024, NewAR, 98, 101694, doi: 10.1016/j.newar.2024.101694
-
[25]
2023a, Monthly Notices of the Royal Astronomical Society, 518, 1057, doi: 10.1093/mnras/stac3140
El-Badry, K., Rix, H.-W., Quataert, E., et al. 2023a, MNRAS, 518, 1057, doi: 10.1093/mnras/stac3140
-
[26]
2023b, Monthly Notices of the Royal Astronomical Society, 521, 4323, doi: 10.1093/mnras/stad799
El-Badry, K., Rix, H.-W., Cendes, Y., et al. 2023b, MNRAS, 521, 4323, doi: 10.1093/mnras/stad799
-
[27]
El-Badry, K., Rix, H.-W., Latham, D. W., et al. 2024, The Open Journal of Astrophysics, 7, 58, doi: 10.33232/001c.121261
-
[28]
Farah, A., Fishbach, M., Essick, R., Holz, D. E., & Galaudage, S. 2022, ApJ, 931, 108, doi: 10.3847/1538-4357/ac5f03
-
[29]
M., Edelman, B., Zevin, M., et al
Farah, A. M., Edelman, B., Zevin, M., et al. 2023, ApJ, 955, 107, doi: 10.3847/1538-4357/aced02
-
[30]
Farah, A. M., Fishbach, M., & Holz, D. E. 2024, ApJ, 962, 69, doi: 10.3847/1538-4357/ad0558
-
[31]
M., Sravan, N., Cantrell, A., et al
Farr, W. M., Sravan, N., Cantrell, A., et al. 2011, ApJ, 741, 103, doi: 10.1088/0004-637X/741/2/103
-
[32]
Fishbach, M., Essick, R., & Holz, D. E. 2020a, ApJL, 899, L8, doi: 10.3847/2041-8213/aba7b6
-
[33]
Fishbach, M., Farr, W. M., & Holz, D. E. 2020b, ApJL, 891, L31, doi: 10.3847/2041-8213/ab77c9
-
[34]
Fishbach, M., & Holz, D. E. 2020, ApJL, 891, L27, doi: 10.3847/2041-8213/ab7247
-
[35]
2022, ApJL, 929, L26, doi: 10.3847/2041-8213/ac64a5
Fishbach, M., & Kalogera, V. 2022, ApJL, 929, L26, doi: 10.3847/2041-8213/ac64a5
-
[36]
L., Belczynski, K., Wiktorowicz, G., et al
Fryer, C. L., Belczynski, K., Wiktorowicz, G., et al. 2012, ApJ, 749, 91, doi: 10.1088/0004-637X/749/1/91
-
[37]
Fryer, C. L., & Kalogera, V. 2001, ApJ, 554, 548, doi: 10.1086/321359 Gaia Collaboration, Prusti, T., de
-
[38]
Bruijne, J. H. J., et al. 2016, A&A, 595, A1, doi: 10.1051/0004-6361/201629272 Gaia Collaboration, Vallenari, A., Brown, A. G. A., et al. 2023, A&A, 674, A1, doi: 10.1051/0004-6361/202243940 Gaia Collaboration, Panuzzo, P., Mazeh, T., et al. 2024, A&A, 686, L2, doi: 10.1051/0004-6361/202449763
-
[39]
Kalogera, V., L Berry, C. P., & Doctor, Z. 2022, ApJL, 938, L19, doi: 10.3847/2041-8213/ac96ef
-
[40]
Hills, J. G. 1983, ApJ, 267, 322, doi: 10.1086/160871
-
[41]
2023a, A&A, 674, A25, doi: 10.1051/0004-6361/202245353 —
Holl, B., Fabricius, C., Portell, J., et al. 2023a, A&A, 674, A25, doi: 10.1051/0004-6361/202245353 —. 2023b, A&A, 674, A25, doi: 10.1051/0004-6361/202245353
-
[42]
2013, MNRAS, 434, 1355, doi: 10.1093/mnras/stt1106
Janka, H.-T. 2013, MNRAS, 434, 1355, doi: 10.1093/mnras/stt1106
-
[43]
2024, Ap&SS, 369, 80, doi: 10.1007/s10509-024-04343-1
Janka, H.-T., & Kresse, D. 2024, Ap&SS, 369, 80, doi: 10.1007/s10509-024-04343-1
-
[44]
2023, A&A, 670, A79, doi: 10.1051/0004-6361/202244818
Marchant, P. 2023, A&A, 670, A79, doi: 10.1051/0004-6361/202244818
-
[45]
1996, ApJ, 471, 352, doi: 10.1086/177974 —
Kalogera, V. 1996, ApJ, 471, 352, doi: 10.1086/177974 —. 2000, ApJ, 541, 319, doi: 10.1086/309400
-
[46]
2024, MNRAS, doi: 10.1093/mnras/stae2591
Kotko, I., Banerjee, S., & Belczynski, K. 2024, MNRAS, 535, 3577, doi: 10.1093/mnras/stae2591
-
[47]
Kreidberg, L., Bailyn, C. D., Farr, W. M., & Kalogera, V. 2012, ApJ, 757, 36, doi: 10.1088/0004-637X/757/1/36
-
[48]
Kruckow, M. U., Andrews, J. J., Fragos, T., et al. 2024, A&A, 692, A141, doi: 10.1051/0004-6361/202452356
-
[49]
Lam, C. Y., El-Badry, K., & Simon, J. D. 2024, arXiv e-prints, arXiv:2411.00654, doi: 10.48550/arXiv.2411.00654
-
[50]
Dawson, W. A., & Golovich, N. R. 2020, ApJ, 889, 31, doi: 10.3847/1538-4357/ab5fd3
-
[51]
Lam, C. Y., Lu, J. R., Udalski, A., et al. 2022, ApJL, 933, L23, doi: 10.3847/2041-8213/ac7442 18 LIGO Scientific Collaboration, Aasi, J.,
-
[52]
Abbott, B. P., et al. 2015, Classical and Quantum Gravity, 32, 074001, doi: 10.1088/0264-9381/32/7/074001
-
[53]
2023, ApJ, 946, 4, doi: 10.3847/1538-4357/acb8b2
Doctor, Z., & Kalogera, V. 2023, ApJ, 946, 4, doi: 10.3847/1538-4357/acb8b2
-
[54]
2021, Research Notes of the American Astronomical Society, 5, 223, doi: 10.3847/2515-5172/ac2d35
Mandel, I. 2021, Research Notes of the American Astronomical Society, 5, 223, doi: 10.3847/2515-5172/ac2d35
-
[55]
2022, PhR, 955, 1, doi: 10.1016/j.physrep.2022.01.003
Mandel, I., & Farmer, A. 2022, PhR, 955, 1, doi: 10.1016/j.physrep.2022.01.003
-
[56]
Mandel, I., Farr, W. M., Colonna, A., et al. 2017, MNRAS, 465, 3254, doi: 10.1093/mnras/stw2883
-
[57]
Mandel, I., & M¨ uller, B. 2020, MNRAS, 499, 3214, doi: 10.1093/mnras/staa3043 Mar´ ın Pina, D., Rastello, S., Gieles, M., et al. 2024, A&A, 688, L2, doi: 10.1051/0004-6361/202450460
-
[58]
Miller, M. C., & Miller, J. M. 2015, PhR, 548, 1, doi: 10.1016/j.physrep.2014.09.003 M¨ uller, B., Gay, D. W., Heger, A., Tauris, T. M., & Sim, S. A. 2018, MNRAS, 479, 3675, doi: 10.1093/mnras/sty1683
-
[59]
2025, PASP, 137, 034203, doi: 10.1088/1538-3873/adb6d6
Nagarajan, P., & El-Badry, K. 2025, PASP, 137, 034203, doi: 10.1088/1538-3873/adb6d6
-
[60]
2025, PASP, 137, 044202, doi: 10.1088/1538-3873/adc839
Nagarajan, P., El-Badry, K., Chawla, C., et al. 2025, PASP, 137, 044202, doi: 10.1088/1538-3873/adc839
-
[61]
Nitz, A. H., Capano, C. D., Kumar, S., et al. 2021, ApJ, 922, 76, doi: 10.3847/1538-4357/ac1c03
-
[62]
2023, ApJ, 953, 152, doi: 10.3847/1538-4357/ace349 O’Shaughnessy, R., Gerosa, D., &
Kalogera, V., & Ye, C. 2023, ApJ, 953, 152, doi: 10.3847/1538-4357/ace349 O’Shaughnessy, R., Gerosa, D., &
-
[63]
2017, PhRvL, 119, 011101, doi: 10.1103/PhysRevLett.119.011101 ¨Ozel, F., Psaltis, D., Narayan, R., &
Wysocki, D. 2017, PhRvL, 119, 011101, doi: 10.1103/PhysRevLett.119.011101 ¨Ozel, F., Psaltis, D., Narayan, R., &
-
[64]
McClintock, J. E. 2010, ApJ, 725, 1918, doi: 10.1088/0004-637X/725/2/1918
-
[65]
Peters, P. C. 1964, Physical Review, 136, 1224, doi: 10.1103/PhysRev.136.B1224
-
[66]
Podsiadlowski, P., Langer, N., Poelarends, A. J. T., et al. 2004, ApJ, 612, 1044, doi: 10.1086/421713
-
[67]
2023, Modern Notices of the Royal Astronomical Society, 526, 740, doi: 10.1093/mnras/stad2757
Rastello, S., Iorio, G., Mapelli, M., et al. 2023, MNRAS, 526, 740, doi: 10.1093/mnras/stad2757
-
[68]
2023, ApJ, 957, 37, doi: 10.3847/1538-4357/acf452
Creighton, J., & Kapadia, S. 2023, ApJ, 957, 37, doi: 10.3847/1538-4357/acf452
-
[69]
Remillard, R. A., & McClintock, J. E. 2006, in American Astronomical Society Meeting Abstracts, Vol. 209, American Astronomical Society Meeting Abstracts, 07.05
work page 2006
-
[70]
Renzo, M., Zapartas, E., de Mink, S. E., et al. 2019, A&A, 624, A66, doi: 10.1051/0004-6361/201833297
-
[71]
Kalogera, V., & Rasio, F. A. 2016, ApJL, 832, L2, doi: 10.3847/2041-8205/832/1/L2
-
[72]
2023, MNRAS, 525, 706, doi: 10.1093/mnras/stad2366
Romagnolo, A., Belczynski, K., Klencki, J., et al. 2023, MNRAS, 525, 706, doi: 10.1093/mnras/stad2366
-
[73]
C., Anderson, J., Casertano, S., et al
Sahu, K. C., Anderson, J., Casertano, S., et al. 2022, ApJ, 933, 83, doi: 10.3847/1538-4357/ac739e
-
[74]
2025, arXiv e-prints, arXiv:2507.05359, doi: 10.48550/arXiv.2507.05359
Sayeed, M., Yang, S., Cinquegrana, G., et al. 2025, arXiv e-prints, arXiv:2507.05359, doi: 10.48550/arXiv.2507.05359
-
[75]
2025, arXiv e-prints, arXiv:2506.16513, doi: 10.48550/arXiv.2506.16513
Shariat, C., El-Badry, K., & Naoz, S. 2025, arXiv e-prints, arXiv:2506.16513, doi: 10.48550/arXiv.2506.16513
-
[76]
2022, Nature Astronomy, 6, 1085, doi: 10.1038/s41550-022-01730-y
Shenar, T., Sana, H., Mahy, L., et al. 2022, Nature Astronomy, 6, 1085, doi: 10.1038/s41550-022-01730-y
-
[77]
C., Kiato, I., Kalogera, V., et al
Siegel, J. C., Kiato, I., Kalogera, V., et al. 2023, ApJ, 954, 212, doi: 10.3847/1538-4357/ace9d9
-
[78]
Formation and Evolution of Compact Stellar X-ray Sources
Tauris, T. M., & van den Heuvel, E. P. J. 2006, in Compact stellar X-ray sources, ed. W. H. G. Lewin & M. van der Klis, Vol. 39, 623–665, doi: 10.48550/arXiv.astro-ph/0303456
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.astro-ph/0303456 2006
-
[79]
2021, ApJL, 913, L19, doi: 10.3847/2041-8213/abfbe7 19
Tiwari, V., & Fairhurst, S. 2021, ApJL, 913, L19, doi: 10.3847/2041-8213/abfbe7 19
-
[80]
Valli, R., de Mink, S. E., Justham, S., et al. 2025, arXiv e-prints, arXiv:2505.08857, doi: 10.48550/arXiv.2505.08857 van Son, L. A. C., de Mink, S. E., Renzo, M., et al. 2022, ApJ, 940, 184, doi: 10.3847/1538-4357/ac9b0a van Son, L. A. C., Roy, S. K., Mandel, I., et al. 2025, ApJ, 979, 209, doi: 10.3847/1538-4357/ada14a
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