REVIEW 3 major objections 6 minor 1 cited by
Comprehensive Radio Monitoring of the Black Hole X-ray Binary Swift J1727.8$-$1613 during its 2023$-$2024 Outburst
T0 review · 3 major / 6 minor · reviewed 2026-08-07 · deepseek-v4-flash
Pith's one-line read The paper assembles 197 epochs of radio monitoring across seven facilities and 0.3–230 GHz to document the complete disk-jet cycle of the black hole X-ray binary Swift J1727 during its 2023–2024 outburst.
desk verdict A genuinely useful, well-documented radio dataset for a landmark BH LMXB outburst; the composite light curve is the soft spot, but the per-facility data release is solid. 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 central object is the composite multi-facility radio light curve spanning 0.3–230 GHz and 197 epochs, with the inter-band spectral index $\alpha$ (defined by $F_\nu \propto \nu^\alpha$) as the diagnostic that labels each accretion state. Because the source is highly variable, the paper computes $\alpha$ only from strictly simultaneous multi-frequency observations taken at a single facility, avoiding cross-telescope angular-scale biases. The light curve itself carries the argument: its shape (plateau, dip, flares, steep decay, re-brightening) is what identifies the quenching, ejection, and reformation of the jet.
What would settle it
Compare simultaneous single-epoch observations from two facilities with different flux calibrators; a reproducible offset larger than the reported statistical errors between them in a non-flaring epoch would show the composite light curve is not one coherent evolution. Alternatively, re-deriving a soft-state spectral index from strictly simultaneous within-facility bands alone and finding it disagrees with the paper's steepest value ($\alpha \approx -1.86$) would falsify the steep-spectrum claim.
Extended reading notes
Core claim
On the paper's own terms, the discovery is that continuous collaborative radio monitoring captured a stellar-mass black hole completing a full accretion-state loop, with the radio flux density and spectral index tracing every stage: a partially self-absorbed compact jet with a flat spectrum ($\alpha \sim 0$) during the hard state, a pre-transition decline attributed to jet quenching, a sequence of discrete ejecta flares with rapidly evolving optically thick-to-thin spectra (including the $\sim 839$ mJy peak at 1.28 GHz on MJD 60231), a soft state dominated by optically thin ejecta whose spectral index varied between $-0.5$ and $-2$ and reached $-1.86 \pm 0.08$ on MJD 60293, and a final hard-state re-brightening with the compact jet re-established. The brightest flaring implies a minimum internal energy $E_{\min} \approx (0.6-2) \times 10^{40}$ erg, at the high end of the range inferred for other sources. The paper further claims that spectral indices steeper than $-1.5$ require electron power-law indices $p > 3$, pointing to an unresolved particle-acceleration problem for black hole jets.
Load-bearing premise
The composite light curve is internally consistent, meaning flux measurements from telescopes with different calibrators, array configurations, and angular resolutions can be combined into a single evolution without large facility-dependent offsets.
Editorial extensions
If this is right
- X-ray, optical, and infrared teams can anchor their observations of this outburst to a common radio timeline, turning the reported state-transition dates into empirically grounded reference points.
- The dataset provides a template for the community to keep releasing comprehensive radio light curves of future low-mass X-ray binary outbursts, just as the paper intends.
- The steep soft-state spectral indices, if confirmed, show that simple optically thin synchrotron emission with standard cooling cannot explain the ejecta, motivating work on particle acceleration and jet-ISM interactions.
- The reported minimum energy of roughly $10^{40}$ erg per flare gives a concrete energy budget for studies of jet feedback in the interstellar medium.
- The multiple flares between MJD 60207 and 60249 support the reading that the source underwent more than one hard-to-soft transition rather than a single one.
Reading between the lines
- A reader might infer that the true 1.28 GHz flare peak could exceed 839 mJy, since the observing cadence sets only a lower bound on the peak flux density.
- If future work quantifies absolute flux-scale offsets between facilities, the flare amplitudes and the soft-state spectral indices, including $\alpha \approx -1.86$, would need to be checked against those systematics before being used as physical constraints.
- The steep-spectrum result, placed next to similar findings in active galaxies, suggests that a common particle-acceleration mechanism may operate across black hole mass scales; that connection is not made by the paper itself.
- The same composite-light-curve approach could be applied to past outbursts where archival multi-facility data already exist, yielding uniform public datasets without requiring new observations.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This paper compiles roughly ten months of radio monitoring of the black hole low-mass X-ray binary Swift J1727.8−1613 from seven facilities (MeerKAT, e-MERLIN, ATA, VLA, ATCA, ALMA, SMA), spanning approximately 0.3-230 GHz. It presents integrated flux densities, per-observatory light curves, and inter-band spectral indices computed only from strictly simultaneous, same-observatory measurements. The authors describe a canonical disk-jet cycle: flat-spectrum compact jet rise, jet quenching with multiple discrete ejecta flares (peak 839.4 mJy at 1.28 GHz), optically thin soft-state decay with steep spectral indices (minimum α = -1.86 ± 0.08), and compact jet reformation near MJD 60385. The primary stated purpose is to provide a public data resource; the data and plotting scripts are released on GitHub and Zenodo.
Significance. If the data are as presented, this is a valuable community resource and a good precedent: it is one of the most comprehensively radio-monitored BH LMXB outbursts, with per-facility light curves and raw data tables. The methodological choice to restrict spectral indices to strictly simultaneous, single-observatory measurements is sound and avoids cross-array angular-scale biases. The paper is appropriately cautious in its interpretation and explicitly defers detailed modeling to future work. The data release with DOI and GitHub is reproducible and will enable multi-wavelength follow-up analyses.
major comments (3)
- [§2.2, Table 1, abstract, conclusion] The manuscript reports inconsistent epoch counts: the abstract states 197 epochs, the conclusion states 198 individual epochs, and §2.2 states that e-MERLIN observed 24 epochs (19 + 5) while Table 1 lists only 22 e-MERLIN entries across the same period. Because Table 1 is the primary data product, please reconcile these numbers and verify that the table contains every epoch represented in the text and figures.
- [§3.1.2] The text says the soft-state re-brightening 'peaked around 2024 January 14 (MJD 60322; ~30 mJy at 1.28 GHz)'. Table 1 lists the nearest MeerKAT 1.28 GHz values as 24.39 ± 0.02 mJy at MJD 60316.332 and 17.72 ± 0.02 mJy at MJD 60323.205, with no 30 mJy point present. Please correct the text or clarify which measurement is being referenced.
- [§3] The paper correctly warns that different telescopes probe different angular scales and that only statistical errors are reported, but it does not quantify the absolute flux-scale systematic errors of the seven facilities. Since Figures 3 and 4 present a composite multi-facility light curve, I request a brief statement or table of typical per-facility flux-scale uncertainties, or a cross-calibration comparison in overlapping frequency and time ranges, so that users can assign a systematic floor when combining the data.
minor comments (6)
- [§1.1, §3.1, Figure 2 caption] The hard-to-soft transition date is written as '2024 October 5' but should be 2023 October 5 for MJD 60222; please fix this in all occurrences.
- [§2.2] 'Almost daily in September 2024' should read September 2023, because the campaign ran from 2023 August through 2024 March.
- [§2.7 and Table 1] The SMA central frequency is given as 225.5 GHz in §2.7 but 225.0 GHz in Table 1; please harmonize.
- [§3.1.1] 'Both the poly and monochromatic light curves' — 'poly' is unclear; consider 'multi-frequency' or 'polychromatic'.
- [Table 1/§3] Consider adding a note near the table or in §3 that the quoted uncertainties are statistical only and that absolute flux-scale uncertainties are of order several percent, so that users do not over-interpret the very small statistical errors (e.g., 0.02-0.03 mJy on bright MeerKAT points).
- [Reference list] The entries 'Russell et al. 2019a' and 'Russell et al. 2019b' are listed with identical journal, volume, page, and DOI (ApJ 883, 198); since both are cited in the text, please correct the duplicate or properly distinguish the two papers.
Circularity Check
No circularity: the paper is a raw-data release whose derived quantities (spectral indices, E_min) use external formalisms and explicit caveats, not fitted inputs renamed as predictions.
full rationale
This paper is an observational data release; its central deliverable is the compiled multi-facility radio light curve of Swift J1727, consisting of directly measured flux densities and strictly simultaneous inter-band spectral indices. No parameter is fitted to a subset of the data and then presented as a prediction of a closely related quantity. The 10 GHz monochromatic light curve is rescaled using the paper's own inter-band spectral index measurements, but the text explicitly labels it as a qualitative description, excludes observations more than an order of magnitude from 10 GHz, and warns that spectral-index variability is an unaccounted systematic, so no forced conclusion follows. The E_min estimates adopt the Fender & Bright (2019) equipartition prescription and literature distances (3.7-5.5 kpc) as external, parameter-free inputs rather than as values tuned to produce a desired result. State-transition timestamps are taken from external Astronomer's Telegrams, and the self-citations that appear (Miller-Jones et al. 2023b localization, Wood et al. 2024/2025 imaging, Hughes et al. 2025 software) concern independent measurements or processing tools, not load-bearing support for the paper's central claim. The cross-facility angular-scale and absolute-flux-scale caveat is disclosed in Section 3 rather than disguised, and because the data are released with per-facility labels and statistical errors only, the composite light curve remains a legitimate observational product. No derivation step reduces by construction to its own inputs, so the appropriate finding is no significant circularity.
Assumptions & free parameters
assumptions (4)
- domain assumption Equipartition between particles and magnetic fields when estimating the minimum internal energy of flares
- domain assumption Distance to Swift J1727 in the range 3.7-5.5 kpc
- domain assumption Flat or inverted radio spectra indicate a partially self-absorbed compact jet (Blandford & Koenigl 1979), and flares indicate discrete jet ejecta
- domain assumption Swift J1727 is a stellar-mass black hole in a low-mass X-ray binary
Cite this review
Pith. "Pith review of Comprehensive Radio Monitoring of the Black Hole X-ray Binary Swift J1727.8$-$1613 during its 2023$-$2024 Outburst." pith.science (2026). https://pith.science/paper/2XRNEDK6
@misc{pith2026250607798,
author = {Pith},
title = {Pith review of: Comprehensive Radio Monitoring of the Black Hole X-ray Binary Swift J1727.8$-$1613 during its 2023$-$2024 Outburst},
year = {2026},
howpublished = {\url{https://pith.science/paper/2XRNEDK6}},
note = {Machine review of arXiv:2506.07798}
}
abstract
This work presents comprehensive multi-frequency radio monitoring of the black hole low-mass X-ray binary Swift J1727.8$-$1613, which underwent its first recorded outburst after its discovery in August 2023. Through a considerable community effort, we have coalesced the data from multiple, distinct observing programs; the light curves include ${\sim} 10$ months and 197 epochs of monitoring from 7 radio facilities with observing frequencies ranging from (approximately) 0.3$-$230GHz. The primary purpose of this work is to provide the broader astronomical community with these light curves to assist with the interpretation of other observing campaigns, particularly non-radio observing frequencies. We discuss the phenomenological evolution of the source, which included: (i) multiple radio flares consistent with the launching of discrete jet ejections, the brightest of which reached $\sim$ 1 Jy; (ii) temporally evolving radio spectral indices ($\alpha$), reaching values steeper than expected for optically-thin synchrotron emission ($\alpha {<} -1$) and emission with significant radiative cooling ($\alpha < -1.5$). We have published a digital copy of the data and intend for this work to set a precedent for the community to continue releasing comprehensive radio light curves of future low-mass X-ray binary outbursts.
Figures
Figures from the paper (4 more)
Forward citations
Cited by 1 Pith paper
-
The Accretion-Ejection Connection in the Black Hole X-ray Binary MAXI J1820$+$070
A four-year multi-wavelength campaign shows tightly correlated radio, X-ray, and optical emission from MAXI J1820, with repeating hard-state re-brightenings that resemble irradiated disk-instability flares.
Reference graph
Works this paper leans on
-
[1]
Bahramian, A., Tremou, E., Tetarenko, A. J., et al. 2023, ApJL, 948, L7, doi: 10.3847/2041-8213/accde1
-
[2]
Ballard, K. R., & Heavens, A. F. 1992, MNRAS, 259, 89, doi: 10.1093/mnras/259.1.89
-
[3]
Barthelmy, S. D., Barbier, L. M., Cummings, J. R., et al. 2005, SSRv, 120, 143, doi: 10.1007/s11214-005-5096-3
-
[4]
Bell, A. R., Matthews, J. H., & Blundell, K. M. 2019, MNRAS, 488, 2466, doi: 10.1093/mnras/stz1805
-
[5]
Belloni, T., M´ endez, M., van der Klis, M., Lewin, W. H. G., & Dieters, S. 1999, ApJL, 519, L159, doi: 10.1086/312130
doi:10.1086/312130 1999
-
[6]
Belloni, T. M. 2010, in Lecture Notes in Physics, ed. T. Belloni, Vol. 794 (Berlin: Springer Verlag), 53, doi: 10.1007/978-3-540-76937-83
-
[7]
Blandford, R. D., & K¨ onigl, A. 1979, ApJ, 232, 34, doi: 10.1086/157262
doi:10.1086/157262 1979
-
[8]
Briggs, D. S. 1995, in American Astronomical Society Meeting Abstracts, Vol. 187, American Astronomical Society Meeting Abstracts, 112.02
1995
Show all 92 references
-
[9]
S., et al
Bright, J. S., et al. 2020, Nature Astron., 4, 697, doi: 10.1038/s41550-020-1023-5
2020 doi
-
[10]
S., Rhodes, L., Farah, W., et al
Bright, J. S., Rhodes, L., Farah, W., et al. 2023, Nature Astronomy, 7, 986, doi: 10.1038/s41550-023-01997-9
2023 doi
-
[11]
P., McCollough, M., et al
Brocksopp, C., Fender, R. P., McCollough, M., et al. 2002, MNRAS, 331, 765, doi: 10.1046/j.1365-8711.2002.05230.x
2002
-
[12]
J., Miller-Jones, J
Burridge, B. J., Miller-Jones, J. C. A., Bahramian, A., et al. 2025, arXiv e-prints, arXiv:2502.06448. https://arxiv.org/abs/2502.06448
2025
- [13]
-
[14]
J., & Corbel, S
Carotenuto, F., Tetarenko, A. J., & Corbel, S. 2022, MNRAS, 511, 4826, doi: 10.1093/mnras/stac329
2022 doi
-
[15]
2021, MNRAS, 504, 444, doi: 10.1093/mnras/stab864 CASA Team, Bean, B., Bhatnagar, S., et al
Carotenuto, F., Corbel, S., Tremou, E., et al. 2021, MNRAS, 504, 444, doi: 10.1093/mnras/stab864 CASA Team, Bean, B., Bhatnagar, S., et al. 2022, PASP, 134, 114501, doi: 10.1088/1538-3873/ac9642
2021 doi
-
[16]
2013, MNRAS, 428, 2500, doi: 10.1093/mnras/sts215
Corbel, S., Coriat, M., Brocksopp, C., et al. 2013, MNRAS, 428, 2500, doi: 10.1093/mnras/sts215
2013 doi
-
[17]
Corbel, S., & Fender, R. P. 2002, ApJL, 573, L35, doi: 10.1086/341870
2002 doi
-
[18]
P., Tzioumis, A
Corbel, S., Fender, R. P., Tzioumis, A. K., et al. 2002, Science, 298, 196, doi: 10.1126/science.1075857
2002 doi
-
[19]
2011, MNRAS, 414, 677, doi: 10.1111/j.1365-2966.2011.18433.x
Coriat, M., Corbel, S., Prat, L., et al. 2011, MNRAS, 414, 677, doi: 10.1111/j.1365-2966.2011.18433.x
2011
-
[21]
A., Miller, J
Draghis, P. A., Miller, J. M., Homan, J., et al. 2023, The Astronomer’s Telegram, 16219, 1
2023
-
[22]
2020, ApJL, 895, L31, doi: 10.3847/2041-8213/ab88b6
Espinasse, M., Corbel, S., Kaaret, P., et al. 2020, ApJL, 895, L31, doi: 10.3847/2041-8213/ab88b6
2020 doi
-
[23]
2010, in Lecture Notes in Physics, ed
Fender, R. 2010, in Lecture Notes in Physics, ed. T. Belloni, Vol. 794 (Berlin: Springer Verlag), 115, doi: 10.1007/978-3-540-76937-85
2010 doi
-
[24]
2019, MNRAS, 489, 4836, doi: 10.1093/mnras/stz2000
Fender, R., & Bright, J. 2019, MNRAS, 489, 4836, doi: 10.1093/mnras/stz2000
2019 doi
-
[25]
2019, MNRAS, 490, L76, doi: 10.1093/mnrasl/slz145
Fender, R., Bright, J., Mooley, K., & Miller-Jones, J. 2019, MNRAS, 490, L76, doi: 10.1093/mnrasl/slz145
2019 doi
-
[26]
1999a, ApJL, 519, L165, doi: 10.1086/312128
Fender, R., Corbel, S., Tzioumis, T., et al. 1999a, ApJL, 519, L165, doi: 10.1086/312128
-
[27]
A., Corbel, S., et al
Fender, R., Woudt, P. A., Corbel, S., et al. 2016, in MeerKAT Science: On the Pathway to the SKA, 13, doi: 10.22323/1.277.0013
2016 doi
-
[28]
P., Belloni, T
Fender, R. P., Belloni, T. M., & Gallo, E. 2004, MNRAS, 355, 1105, doi: 10.1111/j.1365-2966.2004.08384.x
2004
-
[29]
P., Garrington, S
Fender, R. P., Garrington, S. T., McKay, D. J., et al. 1999b, MNRAS, 304, 865, doi: 10.1046/j.1365-8711.1999.02364.x
1999
-
[30]
P., Homan, J., & Belloni, T
Fender, R. P., Homan, J., & Belloni, T. M. 2009, MNRAS, 396, 1370, doi: 10.1111/j.1365-2966.2009.14841.x
2009
-
[31]
2018, MNRAS, 478, L132, doi: 10.1093/mnrasl/sly083
Gallo, E., Degenaar, N., & van den Eijnden, J. 2018, MNRAS, 478, L132, doi: 10.1093/mnrasl/sly083
2018 doi
-
[32]
P., & Pooley, G
Gallo, E., Fender, R. P., & Pooley, G. G. 2003, MNRAS, 344, 60, doi: 10.1046/j.1365-8711.2003.06791.x
2003
-
[33]
2016, Astronomy and Geophysics, 57, 3.28, doi: 10.1093/astrogeo/atw101
Garrington, S., & Beswick, R. 2016, Astronomy and Geophysics, 57, 3.28, doi: 10.1093/astrogeo/atw101
2016 doi
-
[34]
2004, ApJ, 611, 1005, doi: 10.1086/422091
Gehrels, N., Chincarini, G., Giommi, P., et al. 2004, ApJ, 611, 1005, doi: 10.1086/422091
2004 doi
-
[35]
D., Quataert, E., et al
Gottlieb, O., Metzger, B. D., Quataert, E., et al. 2023, ApJL, 958, L33, doi: 10.3847/2041-8213/ad096e
2023 doi
-
[36]
J., & Croston, J
Hardcastle, M. J., & Croston, J. H. 2020, NewAR, 88, 101539, doi: 10.1016/j.newar.2020.101539
2020
-
[37]
2020, oxkat: Semi-automated imaging of MeerKAT observations, Astrophysics Source Code Library, record ascl:2009.003
Heywood, I. 2020, oxkat: Semi-automated imaging of MeerKAT observations, Astrophysics Source Code Library, record ascl:2009.003. http://ascl.net/2009.003
2020
-
[38]
J., Baker, A
Heywood, I., Jarvis, M. J., Baker, A. J., et al. 2016, MNRAS, 460, 4433, doi: 10.1093/mnras/stw1250
2016 doi
-
[39]
J., Hale, C
Heywood, I., Jarvis, M. J., Hale, C. L., et al. 2022, MNRAS, 509, 2150, doi: 10.1093/mnras/stab3021
2022 doi
-
[40]
M., & Johnston, K
Hjellming, R. M., & Johnston, K. J. 1988, ApJ, 328, 600, doi: 10.1086/166318
1988 doi
-
[41]
M., & Rupen, M
Hjellming, R. M., & Rupen, M. P. 1995, Nature, 375, 464, doi: 10.1038/375464a0
1995 doi
-
[42]
2005, Ap&SS, 300, 107, doi: 10.1007/s10509-005-1197-4 30
Homan, J., & Belloni, T. 2005, Ap&SS, 300, 107, doi: 10.1007/s10509-005-1197-4 30
2005 doi
-
[43]
K., Cowie, F
Hughes, A. K., Cowie, F. J., Heywood, I., & Hugo, B. 2025, polkat: Semi-automate full polarization of MeerKAT observations, Astrophysics Source Code Library, record ascl:2502.026
2025
-
[44]
R., & Motta, S
Ingram, A. R., & Motta, S. E. 2019, NewAR, 85, 101524, doi: 10.1016/j.newar.2020.101524
2019
-
[45]
2016, in MeerKAT Science: On the Pathway to the SKA, 1, doi: 10.22323/1.277.0001
Jonas, J., & MeerKAT Team. 2016, in MeerKAT Science: On the Pathway to the SKA, 1, doi: 10.22323/1.277.0001
2016 doi
-
[46]
Kalemci, E., Kara, E., & Tomsick, J. A. 2022, in Handbook of X-ray and Gamma-ray Astrophysics, ed. C. Bambi & A. Sangangelo, 9, doi: 10.1007/978-981-16-4544-0 100-1
2022 doi
-
[47]
A., & Swift Team
Kennea, J. A., & Swift Team. 2023, GRB Coordinates Network, 34540, 1
2023
-
[48]
Koljonen, K. I. I., Russell, D. M., Fern´ andez-Ontiveros, J. A., et al. 2015, ApJ, 814, 139, doi: 10.1088/0004-637X/814/2/139
2015 doi
-
[49]
A., Holland, S
Krimm, H. A., Holland, S. T., Corbet, R. H. D., et al. 2013, ApJS, 209, 14, doi: 10.1088/0067-0049/209/1/14
2013 doi
-
[50]
2015, PhR, 561, 1, doi: 10.1016/j.physrep.2014.09.008
Kumar, P., & Zhang, B. 2015, PhR, 561, 1, doi: 10.1016/j.physrep.2014.09.008
2015 doi
- [51]
-
[52]
2002, Nature, 417, 125, doi: 10.1038/417125a
Livio, M. 2002, Nature, 417, 125, doi: 10.1038/417125a
2002 doi
-
[53]
Longair, M. S. 2011, High Energy Astrophysics (Cambridge University Press)
2011
-
[54]
J., Osler, A., Miller-Jones, J
Maccarone, T. J., Osler, A., Miller-Jones, J. C. A., et al. 2020, MNRAS, 498, L40, doi: 10.1093/mnrasl/slaa120 Mart ´ ı-Vidal, I., Vlemmings, W. H. T., Muller, S., & Casey, S. 2014, A&A, 563, A136, doi: 10.1051/0004-6361/201322633 Mata S´ anchez, D., Mu˜ noz-Darias, T., Armas ...
2020 doi
-
[55]
Casares, J., & Torres, M. A. P. 2024, A&A, 682, L1, doi: 10.1051/0004-6361/202348754 Mata S´ anchez, D., Torres, M. A. P., Casares, J., et al. 2025, A&A, 693, A129, doi: 10.1051/0004-6361/202451960
2024 doi
-
[56]
2009, PASJ, 61, 999, doi: 10.1093/pasj/61.5.999
Matsuoka, M., Kawasaki, K., Ueno, S., et al. 2009, PASJ, 61, 999, doi: 10.1093/pasj/61.5.999
2009 doi
-
[57]
E., & Remillard, R
McClintock, J. E., & Remillard, R. A. 2006, Black hole binaries, Vol. 39 (Cambridge University Press), 157–213
2006
-
[58]
2024, MNRAS, 531, 4893, doi: 10.1093/mnras/stae1393
Mereminskiy, I., Lutovinov, A., Molkov, S., et al. 2024, MNRAS, 531, 4893, doi: 10.1093/mnras/stae1393
2024 doi
-
[59]
A., Miller-Jones, J
Migliari, S., Tomsick, J. A., Miller-Jones, J. C. A., et al. 2010, ApJ, 710, 117, doi: 10.1088/0004-637X/710/1/117
2010 doi
-
[60]
A., et al
Migliori, G., Corbel, S., Tomsick, J. A., et al. 2017, MNRAS, 472, 141, doi: 10.1093/mnras/stx1864
2017 doi
-
[61]
2011, PASJ, 63, S623, doi: 10.1093/pasj/63.sp3.S623
Mihara, T., Nakajima, M., Sugizaki, M., et al. 2011, PASJ, 63, S623, doi: 10.1093/pasj/63.sp3.S623
2011 doi
-
[62]
Miller-Jones, J. C. A., Tetarenko, A. J., Sivakoff, G. R., et al. 2019, Nature, 569, 374, doi: 10.1038/s41586-019-1152-0
2019 doi
-
[63]
F., & Rodr ´ ıguez, L
Mirabel, I. F., & Rodr ´ ıguez, L. F. 1994, Nature, 371, 46, doi: 10.1038/371046a0
1994 doi
-
[64]
2018, in 14th European VLBI Network Symposium & Users Meeting (EVN 2018), 152
Moldon, J. 2018, in 14th European VLBI Network Symposium & Users Meeting (EVN 2018), 152
2018
-
[65]
Offringa, A. R. 2010, AOFlagger: RFI Software. http://ascl.net/1010.017
2010
-
[66]
G., & Roberts, J
Pacholczyk, A. G., & Roberts, J. A. 1971, Physics Today, 24, 57, doi: 10.1063/1.3022939
1971 doi
-
[67]
L., Dichiara, S., Gropp, J
Page, K. L., Dichiara, S., Gropp, J. D., et al. 2023, GRB Coordinates Network, 34537, 1
2023
-
[68]
2024, ApJL, 960, L17, doi: 10.3847/2041-8213/ad17ca
Peng, J.-Q., Zhang, S., Shui, Q.-C., et al. 2024, ApJL, 960, L17, doi: 10.3847/2041-8213/ad17ca
2024 doi
-
[69]
M., Polisensky, E., Clarke, T
Peters, W. M., Polisensky, E., Clarke, T. E., Giacintucci, S., & Kassim, N. E. 2023, The Astronomer’s Telegram, 16279, 1
2023
-
[70]
M., Gallo, E., & Jonker, P
Plotkin, R. M., Gallo, E., & Jonker, P. G. 2013, ApJ, 773, 59, doi: 10.1088/0004-637X/773/1/59
2013 doi
-
[71]
2024, The Astronomer’s Telegram, 16541, 1
Podgorny, J., Svoboda, J., & Dovciak, M. 2024, The Astronomer’s Telegram, 16541, 1
2024
-
[72]
M., Hyman, S
Polisensky, E., Lane, W. M., Hyman, S. D., et al. 2016, ApJ, 832, 60, doi: 10.3847/0004-637X/832/1/60
2016 doi
-
[73]
L., & Tsokaros, A
Ruiz, M., Shapiro, S. L., & Tsokaros, A. 2021, Frontiers in Astronomy and Space Sciences, 8, 39, doi: 10.3389/fspas.2021.656907
2021
-
[74]
P., Miller-Jones, J
Rushton, A. P., Miller-Jones, J. C. A., Curran, P. A., et al. 2017, MNRAS, 468, 2788, doi: 10.1093/mnras/stx526
2017 doi
-
[75]
M., Fender, R
Russell, D. M., Fender, R. P., Hynes, R. I., et al. 2006, MNRAS, 371, 1334, doi: 10.1111/j.1365-2966.2006.10756.x
2006
-
[76]
M., Maitra, D., Dunn, R
Russell, D. M., Maitra, D., Dunn, R. J. H., & Markoff, S. 2010, MNRAS, 405, 1759, doi: 10.1111/j.1365-2966.2010.16547.x
2010
-
[77]
M., Markoff, S., Casella, P., et al
Russell, D. M., Markoff, S., Casella, P., et al. 2013, MNRAS, 429, 815, doi: 10.1093/mnras/sts377
2013 doi
-
[78]
D., Carotenuto, F., Miller-Jones, J
Russell, T. D., Carotenuto, F., Miller-Jones, J. C. A., et al. 2024, The Astronomer’s Telegram, 16552, 1
2024
-
[79]
D., Soria, R., Miller-Jones, J
Russell, T. D., Soria, R., Miller-Jones, J. C. A., et al. 2014, MNRAS, 439, 1390, doi: 10.1093/mnras/stt2498
2014 doi
-
[80]
D., Tetarenko, A
Russell, T. D., Tetarenko, A. J., Miller-Jones, J. C. A., et al. 2019a, ApJ, 883, 198, doi: 10.3847/1538-4357/ab3d36 —. 2019b, ApJ, 883, 198, doi: 10.3847/1538-4357/ab3d36
-
[81]
D., Lucchini, M., Tetarenko, A
Russell, T. D., Lucchini, M., Tetarenko, A. J., et al. 2020, MNRAS, 498, 5772, doi: 10.1093/mnras/staa2650 31 S´ anchez-Sierras, J., & Mu˜ noz-Darias, T. 2020, A&A, 640, L3, doi: 10.1051/0004-6361/202038406
2020 doi
- [82]
-
[83]
M., Zurita, C., et al
Shahbaz, T., Russell, D. M., Zurita, C., et al. 2013, MNRAS, 434, 2696, doi: 10.1093/mnras/stt1212
2013 doi
-
[84]
L., Lightman, A
Shapiro, S. L., Lightman, A. P., & Eardley, D. M. 1976, ApJ, 204, 187, doi: 10.1086/154162
1976 doi
- [85]
-
[86]
M., et al
Tananbaum, H., Gursky, H., Kellogg, E. M., et al. 1972, ApJL, 174, L143, doi: 10.1086/180968
1972 doi
-
[87]
Miller-Jones, J. C. A., & Sivakoff, G. R. 2018, MNRAS, 475, 448, doi: 10.1093/mnras/stx3151
2018 doi
-
[88]
J., Sivakoff, G
Tetarenko, A. J., Sivakoff, G. R., Miller-Jones, J. C. A., et al. 2017, MNRAS, 469, 3141, doi: 10.1093/mnras/stx1048
2017 doi
-
[89]
Gladstone, J. C. 2016, ApJS, 222, 15, doi: 10.3847/0067-0049/222/2/15
2016 doi
-
[90]
S., & Price, R
Thorne, K. S., & Price, R. H. 1975, ApJL, 195, L101, doi: 10.1086/181720 van der Laan, H. 1966, Nature, 211, 1131, doi: 10.1038/2111131a0
1975 doi
-
[91]
M., Miller-Jones, J
Wood, C. M., Miller-Jones, J. C. A., Homan, J., et al. 2021, MNRAS, 505, 3393, doi: 10.1093/mnras/stab1479
2021 doi
- [92]
-
[93]
2023, The Astronomer’s Telegram, 16276, 1
Yu, W. 2023, The Astronomer’s Telegram, 16276, 1
2023
Reviewed August 7, 2026 · model on record in the stance chip above.
Discussion (0). Sign in to comment.