REVIEW 3 major objections 6 minor 66 references
Mass Transfer Physics in Binary Stars and Applications in Gravitational Wave Sources
T0 review · 3 major / 6 minor · reviewed 2026-08-12 · deepseek-v4-flash
Pith's one-line read Revised mass-transfer stability limits make evolved and massive binary donors more stable than older models, shifting double black hole and double white dwarf formation toward stable non-conservative mass transfer.
desk verdict A useful review of the authors' own qcrit work, but the abstract oversells the stable-mass-transfer channel by glossing over its own thermal-timescale caveat. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing object is the adiabatic mass-radius exponent $\zeta_{\rm ad} = d\ln R/d\ln M$ of the donor star, compared with the logarithmic response of its Roche-lobe radius to mass loss. If the donor's radius expands faster than its Roche lobe after removing mass, the overflow runs away on a dynamical timescale and a common envelope forms; if it stays inside the lobe, mass transfer remains stable. The authors computed $\zeta_{\rm ad}$ with realistic, non-polytropic stellar models that respond adiabatically to mass loss, including the partial-ionization effects that matter in evolved giant envelopes, and tabulated the resulting $q_{\rm crit}$ for donors from the main sequence to the asymptotic giant branch and for massive stars.
What would settle it
A sharp test would be a three-dimensional radiation-hydrodynamic simulation of a red supergiant donor at an initial mass ratio just above the paper's $q_{\rm crit}$ for that evolutionary state: if the binary does not enter dynamical-timescale overflow within a few orbital periods, the adiabatic mass-radius threshold has failed there. An observational counterpart would be a mass-transferring binary with donor-to-accretor ratio above the claimed $q_{\rm crit}$ that provably survives without a common envelope.
Extended reading notes
Core claim
The central discovery is a grid of new critical mass ratios $q_{\rm crit}=M_{\rm donor}/M_{\rm accretor}$ for dynamical-timescale mass transfer across essentially the full span of donor star states. For massive main-sequence and Hertzsprung-gap donors, $q_{\rm crit}$ can rise from below 1 to above 20 depending on evolutionary state, far above the traditional constant values of 3–4, so mass transfer in massive binaries is considerably more stable than previously believed. For low- and intermediate-mass red giants and asymptotic giant branch stars, mass transfer is also more stable than polytropic estimates, except that very late asymptotic giant branch stars with $q_{\rm crit}\gtrsim 3$ may lose mass on a thermal timescale through the outer Lagrangian points rather than a prompt dynamical instability. Population synthesis using these thresholds then finds that stable non-conservative mass transfer can dominate the formation of double black holes and explain large mass-ratio systems, and that the first mass transfer phase for double white dwarfs is often stable rather than a common envelope, bringing predicted merger rates and space densities into line with observations.
Load-bearing premise
The load-bearing premise is that a donor star losing mass extremely rapidly responds adiabatically, so instability is decided by the adiabatic mass-radius exponent alone; if real giants and massive stars relax thermally or respond hydrodynamically in ways the adiabatic model does not capture, the revised $q_{\rm crit}$ grid and all downstream population conclusions would need revision.
Editorial extensions
If this is right
- If the revised thresholds are correct, the dominant formation channel for merging double black holes shifts from common-envelope ejection to stable, non-conservative mass transfer during the second mass-transfer phase.
- The observed population of large mass-ratio double black hole mergers receives a natural explanation without invoking dynamical formation in dense clusters or chemically homogeneous evolution.
- Most double white dwarfs would form through a first stable Roche-lobe overflow followed by one common-envelope phase, matching the observed double white dwarf space density and merger rate per galaxy.
- The upper ends of observed mass-ratio distributions in X-ray binaries and cataclysmic variables should trace the newly tabulated $q_{\rm crit}$ curves, providing a direct observational check.
- The Galactic type Ia supernova rate implied by the double white dwarf channel also comes into agreement with observations, tying the stability thresholds to cosmological distance measurements.
Reading between the lines
- A consequence the authors leave implicit is that common-envelope efficiency loses much of its leverage over predicted compact-object merger rates; the uncertain parameters that now dominate are the mass fraction and angular momentum carried away during stable non-conservative transfer.
- If the adiabatic thresholds hold, many binaries previously destined to merge inside a common envelope should instead survive as wider, long-lived systems; counting such wide double compact objects in future astrometric surveys would test the shift.
- The same mass-radius-response criterion could be extended to rapidly rotating or magnetized donors, whose adiabatic exponents and Roche-lobe geometry differ, producing subpopulation-dependent $q_{\rm crit}$ values.
- The adiabatic assumption is most fragile in the partially ionized envelopes of late asymptotic giant branch stars, where thermal relaxation may compete with dynamical response; targeted hydrodynamic simulations there would be the sharpest check.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This manuscript, a proceedings contribution for IAU Symposium 389, reviews the authors' adiabatic mass-loss model for computing critical mass ratios (qcrit) for dynamical-timescale mass transfer in binary stars, and summarizes claimed applications to gravitational-wave source populations. It argues that mass transfer in red giant, asymptotic giant branch, and massive stars is more stable than earlier polytropic models suggested, and reports that when these updated thresholds are used in population synthesis, non-conservative stable mass transfer may dominate the formation of double black holes and may reconcile observed double white dwarf merger rates. The paper contains no new derivations, data, or error estimates; its content is a summary of prior work by Ge et al. and others.
Significance. The underlying program is significant: the revised qcrit thresholds are already used by several independent groups (e.g., Neijssel et al. 2019; Gallegos-Garcia et al. 2021; Marchant et al. 2021; Picco et al. 2024) and have received partial independent confirmation through Temmink et al. (2023) and through comparisons with observed mass-ratio upper limits in cataclysmic variables and X-ray binaries. The manuscript itself is a concise review, and its value lies in summarizing the current state of a research program rather than presenting new results. The central application claims are plausible but depend on a number of assumptions, most notably the treatment of thermal-timescale stability, which are not adequately addressed in the manuscript.
major comments (3)
- [Section 2, last paragraph; Sections 3 and 4] The manuscript states in Section 2 that 'The unstable mass transfer for late RGB/AGB stars with qcrit >~ 3 might be dominated by a thermal timescale (shorter than 100 yrs) process through outer Lagrangian points ... instead of a prompt dynamical timescale case.' Yet the applications in Sections 3 and 4 present population synthesis results (Neijssel et al. 2019; Li et al. 2023; Picco et al. 2024) that use qcrit as a binary switch between common-envelope evolution and stable non-conservative Roche-lobe overflow. For donors that are dynamically stable by the adiabatic criterion but thermally unstable on the 10^2 to 10^4 yr timescale, this switch misclassifies the mass transfer outcome, and the overlap between the q<qcrit stable window and the thermally unstable regime is not quantified. The authors should either specify which of the cited syntheses include a separate thermal-stability check, or moderate the claims that non-conservative stable mass transfer dominates the BBH formation channel and reconciles the DWD merger rate.
- [Section 4] The DWD application relies almost exclusively on Li et al. (2023), a population synthesis study by the same group (including H. Ge and Z. Han as co-authors). The paper's phrasing—'Ge et al.'s results support the observational DWDs merger rate distribution'—presents a model-dependent interpretation as a robust confirmation. The manuscript should clarify that the DWD merger-rate match is a prediction of one specific synthesis code with several additional assumptions (e.g., common-envelope efficiency, angular-momentum loss prescriptions) and note whether any independent group has reproduced this result.
- [Section 3] The abstract and Section 3 claim that non-conservative stable mass transfer can explain the population of large-mass-ratio double stellar-mass black holes, but the paper provides no quantitative comparison with the observed GWTC-3 mass-ratio distribution or merger-rate measurements; it only cites Picco et al. (2024). If the authors wish to make this a headline claim of the review, they should show a figure or table comparing predicted and observed mass-ratio distributions, or explicitly label the claim as an interpretation from a cited population synthesis study rather than an established result of the present program.
minor comments (6)
- [Abstract] The phrase 'binary population thesis studies' should be 'binary population synthesis studies,' and 'predicate' should be 'predict.'
- [Section 2] The word 'overcom' should be 'overcome,' and the sentence 'For RGB/AGB HG low- and intermediate mass stars' contains a misplaced abbreviation; it should likely read 'For low- and intermediate mass stars in the HG/RGB/AGB phases.'
- [Figure 1] Figure 1 is extremely dense and nearly unreadable at print size; splitting it into multiple panels or providing a higher-resolution version would improve clarity.
- [Figure 3] The caption refers to 'color lines' but no color legend is provided in the text; please add a legend or describe the line styles.
- [References] Several citations are to arXiv preprints (e.g., Ge et al. 2024, Li et al. 2024); if these have been accepted for publication, please update the references accordingly.
- [Throughout] The abbreviation 'smBH' is used inconsistently with 'stellar-mass black hole' in full; please define and use abbreviations consistently.
Circularity Check
No significant circularity: the qcrit thresholds are independently derived and externally benchmarked, and the downstream applications use external population-synthesis codes and observational comparisons.
full rationale
The paper's central quantity, the dynamical-timescale mass-transfer threshold qcrit, is obtained from an adiabatic mass-loss model using realistic stellar models (Ge et al. 2010a,b, 2015, 2020), not from the gravitational-wave or DWD observations it is later compared with. The text reports external confirmation by Temmink et al. (2023) for low- and intermediate-mass stars, and the BBH application cites independent population-synthesis studies (Neijssel et al. 2019; Picco et al. 2024; etc.) that adopt the thresholds as input and compare with LIGO/Virgo data. The DWD section leans on Li et al. (2023), a same-group population-synthesis study that uses Ge et al.'s thresholds; however, that study is checked against observed DWD space densities and merger rates, so the support is an external-data consistency test rather than an equivalence-by-construction or a fitted-input-renamed-as-prediction. No equation in the paper is defined in terms of the conclusions, and no parameter is fitted to the target data and then called a prediction. Accordingly, no circular step meeting the evidentiary bar can be quoted.
Assumptions & free parameters
assumptions (4)
- domain assumption Adiabatic approximation for rapid mass transfer
- domain assumption Dynamical stability is set by comparing donor mass-radius response with Roche-lobe response
- domain assumption Common-envelope evolution treatment as referenced
- domain assumption Cited population synthesis models are representative
Cite this review
Pith. "Pith review of Mass Transfer Physics in Binary Stars and Applications in Gravitational Wave Sources." pith.science (2026). https://pith.science/paper/WJYB36NA
@misc{pith2026241117333,
author = {Pith},
title = {Pith review of: Mass Transfer Physics in Binary Stars and Applications in Gravitational Wave Sources},
year = {2026},
howpublished = {\url{https://pith.science/paper/WJYB36NA}},
note = {Machine review of arXiv:2411.17333}
}
read the original abstract
The stability criteria of rapid mass transfer and common-envelope evolution are fundamental in binary star evolution. They determine the mass, mass ratio, and orbital distribution of many important systems, such as X-ray binaries, type Ia supernovae, and merging gravitational-wave sources. In the limit of extremely rapid mass transfer, the response of a donor star in an interacting binary becomes asymptotically one of adiabatic expansion. We built the adiabatic mass-loss model and systematically surveyed the thresholds for dynamical timescale mass transfer over the entire span of possible donor star evolutionary states. Many studies indicate that new mass transfer stability thresholds play an essential role in the formation and properties of double compact object populations and the progenitors of SNe Ia and detectable GW sources. For example, our studies show that the mass transfer in the red giant and the asymptotic giant branch stars and the massive stars can be more stable than previously believed. Consequently, detailed binary population synthesis studies, using updated unstable mass transfer criteria, predicate the non-conservative stable mass transfer may dominate the formation channel of double stellar-mass black holes and can explain the population of the large mass ratio double stellar-mass black holes. Using our updated mass transfer thresholds, binary population thesis studies by Li et al. show that Ge et al.'s results support the observational double white dwarfs merger rate distribution per Galaxy and the space density of double white dwarfs in the Galaxy.
Figures
Figures from the paper (1 more)
Reference graph
Works this paper leans on
-
[1]
Abbott B. P., Abbott R., Abbott T. D., Abernathy M. R., Acernese F., Ackley K., Adams C., et al., 2016, PhRvL, 116, 061102. doi:10.1103/PhysRevLett.116.061102
-
[2]
D., Abraham S., Acernese F., Ackley K., Adams C., Adhikari R
Abbott R., Abbott T. D., Abraham S., Acernese F., Ackley K., Adams C., Adhikari R. X., et al., 2020, PhRvL, 125, 101102. doi:10.1103/PhysRevLett.125.101102
-
[3]
D., Abraham S., Acernese F., Ackley K., Adams C., Adhikari R
Abbott R., Abbott T. D., Abraham S., Acernese F., Ackley K., Adams C., Adhikari R. X., et al., 2020, ApJL, 896, L44. doi:10.3847/2041-8213/ab960f
-
[4]
D., Acernese F., Ackley K., Adams C., Adhikari N., Adhikari R
Abbott R., Abbott T. D., Acernese F., Ackley K., Adams C., Adhikari N., Adhikari R. X., et al., 2023, PhRvX, 13, 041039. doi:10.1103/PhysRevX.13.041039
-
[5]
Agazie G., Anumarlapudi A., Archibald A. M., Arzoumanian Z., Baker P. T., B \'e csy B., Blecha L., et al., 2023, ApJL, 951, L8. doi:10.3847/2041-8213/acdac6
-
[6]
doi:10.1007/s41114-022-00041-y
Amaro-Seoane P., Andrews J., Arca Sedda M., Askar A., Baghi Q., Balasov R., Bartos I., et al., 2023, LRR, 26, 2. doi:10.1007/s41114-022-00041-y
-
[7]
Belczynski K., Kalogera V., Bulik T., 2002, ApJ, 572, 407. doi:10.1086/340304
doi:10.1086/340304 2002
-
[8]
Briel M. M., Stevance H. F., Eldridge J. J., 2023, MNRAS, 520, 5724. doi:10.1093/mnras/stad399
Show all 66 references
-
[9]
R., Kilic M., Kosakowski A., Andrews J
Brown W. R., Kilic M., Kosakowski A., Andrews J. J., Heinke C. O., Ag \"u eros M. A., Camilo F., et al., 2020, ApJ, 889, 49. doi:10.3847/1538-4357/ab63cd
2020 doi
-
[10]
doi:10.1046/j.1365-8711.2003.06449.x
Chen X., Han Z., 2003, MNRAS, 341, 662. doi:10.1046/j.1365-8711.2003.06449.x
2003
-
[11]
doi:10.1111/j.1365-2966.2008.13334.x
Chen X., Han Z., 2008, MNRAS, 387, 1416. doi:10.1111/j.1365-2966.2008.13334.x
2008
-
[12]
M., 2021, MNRAS, 506, 2269
El-Badry K., Rix H.-W., Heintz T. M., 2021, MNRAS, 506, 2269. doi:10.1093/mnras/stab323
2021 doi
-
[13]
doi:10.1051/0004-6361/202346844
EPTA Collaboration, InPTA Collaboration, Antoniadis J., Arumugam P., Arumugam S., Babak S., Bagchi M., et al., 2023, A&A, 678, A50. doi:10.1051/0004-6361/202346844
2023 doi
-
[14]
Gallegos-Garcia M., Berry C. P. L., Marchant P., Kalogera V., 2021, ApJ, 922, 110. doi:10.3847/1538-4357/ac2610
2021 doi
-
[15]
S., Webbink R
Ge H., Hjellming M. S., Webbink R. F., Chen X., Han Z., 2010, ApJ, 717, 724. doi:10.1088/0004-637X/717/2/724
2010 doi
-
[16]
F., Chen X., Han Z., 2015, ApJ, 812, 40
Ge H., Webbink R. F., Chen X., Han Z., 2015, ApJ, 812, 40. doi:10.1088/0004-637X/812/1/40
2015 doi
-
[17]
F., Chen X., Han Z., 2020, ApJ, 899, 132
Ge H., Webbink R. F., Chen X., Han Z., 2020, ApJ, 899, 132. doi:10.3847/1538-4357/aba7b7
2020 doi
-
[18]
F., Han Z., 2020, ApJS, 249, 9
Ge H., Webbink R. F., Han Z., 2020, ApJS, 249, 9. doi:10.3847/1538-4365/ab98f6
2020 doi
-
[19]
F., Han Z., Chen X., 2010, Ap&SS, 329, 243
Ge H., Webbink R. F., Han Z., Chen X., 2010, Ap&SS, 329, 243. doi:10.1007/s10509-010-0286-1
2010 doi
-
[20]
A., Chen X., Sarkar A., Walton D
Ge H., Tout C. A., Chen X., Sarkar A., Walton D. J., Han Z., 2023, ApJ, 945, 7. doi:10.3847/1538-4357/acb7e9
2023 doi
- [21]
-
[22]
Han Z., 2003, ASPC, 289, 413
2003
-
[23]
doi:10.1088/1674-4527/20/10/161
Han Z.-W., Ge H.-W., Chen X.-F., Chen H.-L., 2020, RAA, 20, 161. doi:10.1088/1674-4527/20/10/161
2020 doi
- [24]
- [25]
-
[26]
doi:10.1051/0004-6361/202243893
Li Z., Chen X., Ge H., Chen H.-L., Han Z., 2023, A&A, 669, A82. doi:10.1051/0004-6361/202243893
2023 doi
-
[27]
doi:10.1051/0004-6361/201833010
Liu D., Wang B., Ge H., Chen X., Han Z., 2019, A&A, 622, A35. doi:10.1051/0004-6361/201833010
2019 doi
-
[28]
doi:10.1051/0004-6361:20030512
Meynet G., Maeder A., 2003, A&A, 404, 975. doi:10.1051/0004-6361:20030512
2003 doi
-
[29]
E., 2016, MNRAS, 458, 2634
Mandel I., de Mink S. E., 2016, MNRAS, 458, 2634. doi:10.1093/mnras/stw379
2016 doi
-
[30]
E., Vigna-G \'o mez A., Chattopadhyay D., 2021, MNRAS, 500, 1380
Mandel I., M \"u ller B., Riley J., de Mink S. E., Vigna-G \'o mez A., Chattopadhyay D., 2021, MNRAS, 500, 1380. doi:10.1093/mnras/staa3390
2021 doi
-
[31]
doi:10.1093/mnras/sty339
Maoz D., Hallakoun N., Badenes C., 2018, MNRAS, 476, 2584. doi:10.1093/mnras/sty339
2018 doi
- [32]
-
[33]
M., Moriya T
Marchant P., Langer N., Podsiadlowski P., Tauris T. M., Moriya T. J., 2016, A&A, 588, A50. doi:10.1051/0004-6361/201628133
2016 doi
-
[34]
Marchant P., Pappas K. M. W., Gallegos-Garcia M., Berry C. P. L., Taam R. E., Kalogera V., Podsiadlowski P., 2021, A&A, 650, A107. doi:10.1051/0004-6361/202039992
2021 doi
-
[35]
J., Vigna-G \'o mez A., Stevenson S., Barrett J
Neijssel C. J., Vigna-G \'o mez A., Stevenson S., Barrett J. W., Gaebel S. M., Broekgaarden F. S., de Mink S. E., et al., 2019, MNRAS, 490, 3740. doi:10.1093/mnras/stz2840
2019 doi
-
[36]
W., Tremblay P.-E., Klein B
O'Brien M. W., Tremblay P.-E., Klein B. L., Koester D., Melis C., B \'e dard A., Cukanovaite E., et al., 2024, MNRAS, 527, 8687. doi:10.1093/mnras/stad3773
2024 doi
-
[37]
doi:10.1051/0004-6361/202140520
Olejak A., Belczynski K., Ivanova N., 2021, A&A, 651, A100. doi:10.1051/0004-6361/202140520
2021 doi
-
[38]
doi:10.1051/0004-6361/202450480
Olejak A., Klencki J., Xu X.-T., Wang C., Belczynski K., Lasota J.-P., 2024, A&A, 689, A305. doi:10.1051/0004-6361/202450480
2024 doi
-
[39]
Paczynski B., 1976, IAUS, 73, 75
1976
-
[40]
F., G \"a nsicke B
Pala A. F., G \"a nsicke B. T., Breedt E., Knigge C., Hermes J. J., Gentile Fusillo N. P., Hollands M. A., et al., 2020, MNRAS, 494, 3799. doi:10.1093/mnras/staa764
2020 doi
-
[41]
doi:10.1093/mnras/stv619
Pavlovskii K., Ivanova N., 2015, MNRAS, 449, 4415. doi:10.1093/mnras/stv619
2015 doi
-
[42]
X., 2017, MNRAS, 465, 2092
Pavlovskii K., Ivanova N., Belczynski K., Van K. X., 2017, MNRAS, 465, 2092. doi:10.1093/mnras/stw2786
2017 doi
-
[43]
A., Nugent P., Castro P
Perlmutter S., Aldering G., Goldhaber G., Knop R. A., Nugent P., Castro P. G., Deustua S., et al., 1999, ApJ, 517, 565. doi:10.1086/307221
1999 doi
-
[44]
doi:10.1051/0004-6361/202347090
Picco A., Marchant P., Sana H., Nelemans G., 2024, A&A, 681, A31. doi:10.1051/0004-6361/202347090
2024 doi
-
[45]
F., McMillan S
Portegies Zwart S. F., McMillan S. L. W., 2000, ApJL, 528, L17. doi:10.1086/312422
2000 doi
-
[46]
M., Torres S., Rodrigo C., Ferrer-Burjachs A., Calcaferro L
Rebassa-Mansergas A., Solano E., Jim \'e nez-Esteban F. M., Torres S., Rodrigo C., Ferrer-Burjachs A., Calcaferro L. M., et al., 2021, MNRAS, 506, 5201. doi:10.1093/mnras/stab2039
2021 doi
-
[47]
J., Zic A., Shannon R
Reardon D. J., Zic A., Shannon R. M., Hobbs G. B., Bailes M., Di Marco V., Kapur A., et al., 2023, ApJL, 951, L6. doi:10.3847/2041-8213/acdd02
2023 doi
-
[48]
S., Parsons S
Ren J.-J., Raddi R., Rebassa-Mansergas A., Hernandez M. S., Parsons S. G., Irawati P., Rittipruk P., et al., 2020, ApJ, 905, 38. doi:10.3847/1538-4357/abc017
2020 doi
-
[49]
G., Filippenko A
Riess A. G., Filippenko A. V., Challis P., Clocchiatti A., Diercks A., Garnavich P. M., Gilliland R. L., et al., 1998, AJ, 116, 1009. doi:10.1086/300499
1998 doi
-
[50]
G., Strolger L.-G., Tonry J., Casertano S., Ferguson H
Riess A. G., Strolger L.-G., Tonry J., Casertano S., Ferguson H. C., Mobasher B., Challis P., et al., 2004, ApJ, 607, 665. doi:10.1086/383612
2004 doi
-
[51]
doi:10.1088/0004-637X/796/1/37
Shao Y., Li X.-D., 2014, ApJ, 796, 37. doi:10.1088/0004-637X/796/1/37
2014 doi
-
[52]
doi:10.3847/1538-4357/ac173e
Shao Y., Li X.-D., 2021, ApJ, 920, 81. doi:10.3847/1538-4357/ac173e
2021 doi
- [53]
- [54]
-
[55]
D., Pols O
Temmink K. D., Pols O. R., Justham S., Istrate A. G., Toonen S., 2023, A&A, 669, A45. doi:10.1051/0004-6361/202244137
2023 doi
-
[56]
L., Schmidt B
Tonry J. L., Schmidt B. P., Barris B., Candia P., Challis P., Clocchiatti A., Coil A. L., et al., 2003, ApJ, 594, 1. doi:10.1086/376865
2003 doi
-
[57]
van Son L. A. C., de Mink S. E., Callister T., Justham S., Renzo M., Wagg T., Broekgaarden F. S., et al., 2022, ApJ, 931, 17. doi:10.3847/1538-4357/ac64a3
2022 doi
-
[58]
van Son L. A. C., de Mink S. E., Renzo M., Justham S., Zapartas E., Breivik K., Callister T., et al., 2022, ApJ, 940, 184. doi:10.3847/1538-4357/ac9b0a
2022 doi
-
[59]
F., 1975, PhDT
Webbink R. F., 1975, PhDT
1975
-
[60]
F., 1985, ibs..book, 39
Webbink R. F., 1985, ibs..book, 39
1985
-
[61]
doi:10.3847/1538-4357/acffb1
Willcox R., MacLeod M., Mandel I., Hirai R., 2023, ApJ, 958, 138. doi:10.3847/1538-4357/acffb1
2023 doi
-
[62]
doi:10.3847/2041-8213/ac2cc8
Willcox R., Mandel I., Thrane E., Deller A., Stevenson S., Vigna-G \'o mez A., 2021, ApJL, 920, L37. doi:10.3847/2041-8213/ac2cc8
2021 doi
-
[63]
doi:10.1088/1674-4527/acdfa5
Xu H., Chen S., Guo Y., Jiang J., Wang B., Xu J., Xue Z., et al., 2023, RAA, 23, 075024. doi:10.1088/1674-4527/acdfa5
2023 doi
-
[64]
R., Shahaf S., Mazeh T., Andrae R., 2024, PASP, 136, 084202
Yamaguchi N., El-Badry K., Rees N. R., Shahaf S., Mazeh T., Andrae R., 2024, PASP, 136, 084202. doi:10.1088/1538-3873/ad6809
2024 doi
-
[65]
doi:10.3847/1538-4365/ad6263
Zhang L., Ge H., Chen X., Han Z., 2024, ApJS, 274, 11. doi:10.3847/1538-4365/ad6263
2024 doi
-
[66]
write newline
" write newline "" before.all 'output.state := FUNCTION fin.entry add.period write newline FUNCTION new.block output.state before.all = 'skip after.block 'output.state := if FUNCTION new.sentence output.state after.block = 'skip output.state before.all = 'skip after.sentence '...
Reviewed August 12, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.