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arxiv: 2601.11784 · v2 · submitted 2026-01-16 · 🌌 astro-ph.HE

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Einstein Probe discovery of EP J171159.4-333253: an eclipsing neutron star low-mass X-ray binary with clocked bursts

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Pith reviewed 2026-05-16 13:01 UTC · model grok-4.3

classification 🌌 astro-ph.HE
keywords neutron starlow-mass X-ray binarytype-I X-ray burstseclipsesorbital periodhelium burstsEinstein ProbeNuSTAR
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The pith

A new neutron star low-mass X-ray binary shows clocked type-I bursts recurring every 8196 seconds along with eclipses.

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

The paper reports the discovery of EP J171159.4-333253 as an eclipsing neutron-star low-mass X-ray binary in outburst, detected by the Einstein Probe. It measures a burst recurrence time of 8196 plus or minus 177 seconds from nine events, an orbital period of 6.48301 hours from eclipse timings, and an eclipse duration of about 1245 seconds. These data yield estimates for the companion star mass of 0.6 to 0.8 solar masses, radius of 0.7 to 0.8 solar radii, and binary inclination of 73 to 75 degrees. A reader would care because the regular timing and multiwavelength coverage allow direct constraints on thermonuclear burning and accretion flow geometry in such systems. The persistent emission is typical of a hard state, and the accretion-to-thermonuclear energy ratio of 120 to 130 points to helium bursts after hydrogen depletion between events.

Core claim

EP J171159.4-333253 is a neutron-star low-mass X-ray binary exhibiting clocked type-I X-ray bursts with a recurrence time of 8196 plus or minus 177 seconds over a nine-burst subset, eclipses with duration 1245.5 plus 6.9 minus 6.5 seconds, and an orbital period of 6.48301 plus or minus 0.00003 hours. These enable companion mass and radius estimates of 0.6 to 0.8 solar masses and 0.7 to 0.8 solar radii at inclination 73 to 75 degrees. The accretion-to-thermonuclear energy ratio of 120 to 130 implies helium bursts with accreted hydrogen depleted between events.

What carries the argument

The clocked X-ray bursts with measured recurrence time together with the X-ray eclipse events that fix the orbital period, eclipse duration, and derived companion properties.

If this is right

  • The source remains in a hard spectral state with typical persistent X-ray emission properties despite moderate flux variation.
  • The optical eclipse is broader and wavelength-dependent compared to the X-ray eclipse, showing that part of the optical emission comes from an extended region in the accretion flow.
  • The measured energy ratio indicates helium ignition bursts once accreted hydrogen is depleted between events.

Where Pith is reading between the lines

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

  • Longer-term monitoring could test whether the possible decreasing trend in recurrence time continues and how it depends on changing accretion rate.
  • The joint X-ray and optical eclipse coverage offers a way to map vertical structure in the accretion disk or corona.
  • This source adds a well-timed example that could help calibrate population models for eclipsing neutron-star LMXBs if similar systems are found at comparable distances.

Load-bearing premise

The observed periodic X-ray dips are true eclipses by the companion star rather than disk structures or other variability, and the nine-burst subset fully represents the recurrence behavior without undetected events or strong secular changes.

What would settle it

Detection of one or more X-ray bursts occurring well outside the predicted 8196-second recurrence window or spectroscopic or timing evidence that the dips arise from accretion disk structures instead of the companion star.

Figures

Figures reproduced from arXiv: 2601.11784 by A. Marino, A. Papitto, A. Patruno, B. F. Liu, C. C. Jin, E. Parent, F. Ambrosino, F. Coti Zelati, G. B. Zhang, G. Illiano, H. Feng, H. N. Yang, H. Q. Cheng, H. Sun, I. Ribas, J. Blanco-Pozo, J. H. Wu, J. W. Hu, K. R. Ni, L. Tao, N. Rea, Q. C. Zhao, S. Guillot, S. P. Littlefair, V. S. Dhillon, W. Yuan, Y. Cavecchi, Y. J. Xu, Y. L. Wang, Z. H. Yang.

Figure 1
Figure 1. Figure 1: X-ray light curve of EP J1711−3332 extracted from EP/WXT data collected during the first 21 days of the outburst. Observed fluxes refer to the 0.5–4 keV energy range and were obtained by combining data from snapshots taken on the same day. The shaded gray area marks the epoch of the NuSTAR observation. 2.1. Einstein Probe 2.1.1. Wide-field X-ray Telescope (WXT) The WXT on board EP (W. Yuan et al. 2022) is … view at source ↗
Figure 2
Figure 2. Figure 2: X-ray light curve of EP J1711−3332 obtained in the NuSTAR observation. The dot-dashed gray lines mark the expected epochs of bursts, using the epoch of the fourth burst as a reference and assuming a constant trec of 8200 s. The expected ingress (dashed blue lines) and egress (dotted red lines) epochs of eclipses are calculated from ObsID 11900304129 ( [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Left: measured recurrence times trec (black) for the eight consecutive pairs of bursts with unambiguous cycle counts. The grey shaded regions denote the validity range of each measurement, extending from the start of one burst to the start of the subsequent burst. The first burst in the first trec measurement corresponds to burst No. 3 in Table B2, while the final burst in the last measurement corresponds … view at source ↗
Figure 4
Figure 4. Figure 4: X-ray light curve of EP J1711−3332 from Ob￾sID 11900304129. This is the only EP/FXT observation where an entire eclipse event was captured. We use the ingress and egress epochs observed in this eclipse event as reference points to calculate the expected ingress and egress epochs in other observations. See Figure B2 for all the FXT light curves. σD = 14.0 s (95% upper limit: 68.6 s). Uncertainties rep￾resen… view at source ↗
Figure 5
Figure 5. Figure 5: Phase-resolved light curves of four EP/FXT observations with dips (orange hatched bands). Each panel shows the data obtained over one orbit of the binary system. The orbit observed by the first FXT observation is defined as Orbit 1. The expected ingress (dashed blue lines) and egress (dotted red lines) epochs are calculated from ObsID 11900304129. The shaded gray area is the observed eclipse period. See Fi… view at source ↗
Figure 6
Figure 6. Figure 6: Broadband EP/FXT (blue) and NuSTAR (green) spectra with the best-fit Model 1 (top panel), and residuals from Model 0 (middle panel) and Model 1 (bottom panel). The EP/FXT data are from ObsIDs 0680000699 (Epoch 1), 0680000706 (Epoch 2) and 0680000707 (Epoch 3). Different line styles were adopted to distinguish different components: dot for diskbb, dash for thcomp×bbodyrad and dash-dot for relxillCp. der to … view at source ↗
Figure 7
Figure 7. Figure 7 [PITH_FULL_IMAGE:figures/full_fig_p010_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: A deep stack of the 2.2 hours of optical data obtained with ULTRACAM in the gs (top) and is (bottom) bands. The 785 images were individually shifted to account for image motion prior to adding together. The images shown are 30′′ on a side. North is up and East to the left. The optical counterpart is indicated with the red tick marks. The positional error regions of the X-ray source (EP/FXT) and the radio c… view at source ↗
read the original abstract

EP J171159.4-333253 is a new neutron-star low-mass X-ray binary discovered in outburst by the Einstein Probe (EP) on 2025 June 23, exhibiting clocked type-I X-ray bursts, eclipses and dips. In this paper, we report on the results of the X-ray spectral and timing analyses for EP J171159.4-333253 using data collected by EP and NuSTAR during the first 21 days of the outburst. The X-ray burst recurrence time can be characterized over a subset of nine bursts spanning 1.6 days around the NuSTAR observation, and the result is $t_{\rm rec}=8196 \pm 177\,$s with indications of a possible decreasing trend. From the X-ray eclipse events, the binary orbital period and the eclipse duration are estimated to be $P_{\rm orb}=6.48301 \pm 0.00003\,$hr and $D_{\star,X} = 1245.5^{+6.9}_{-6.5}\,$s, respectively. These enable an estimate of the mass and radius of the companion star and the binary inclination, which are $M_2\approx0.6-0.8\,M_\odot$, $R_2\approx0.7-0.8\,R_\odot$ and $i\approx73-75^\circ$, respectively. We also report on joint ULTRACAM and EP observations on 2025 July 21--22, detecting the source optical counterpart and covering an eclipse in both X-ray and optical bands. The optical eclipse is wavelength-dependent and broader than in X-rays, indicating that part of the optical emission arises from an extended region in the accretion flow. Despite a moderate variation in the source flux, the properties of the persistent X-ray emission are typical of a hard spectral state. We further evaluated the ratio of the accretion energy to the thermonuclear energy to be 120--130, implying helium bursts with the accreted hydrogen being depleted in-between bursts.

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 manuscript presents the discovery of EP J171159.4-333253, a new neutron-star low-mass X-ray binary found in outburst by the Einstein Probe. It exhibits clocked type-I X-ray bursts, eclipses, and dips. Key results include a burst recurrence time of 8196 ± 177 s from nine events over 1.6 days, an orbital period of 6.48301 ± 0.00003 hr, an X-ray eclipse duration of 1245.5 +6.9 -6.5 s, companion star mass and radius estimates of approximately 0.6-0.8 solar masses and 0.7-0.8 solar radii, an inclination of 73-75 degrees, and an accretion-to-thermonuclear energy ratio of 120-130 suggesting helium bursts. Joint optical observations confirm the counterpart and show a wavelength-dependent eclipse.

Significance. This discovery contributes to the limited sample of eclipsing clocked bursters, offering precise measurements of orbital and burst parameters that can test models of thermonuclear ignition and binary evolution. The use of multiple instruments and the optical data provide a comprehensive view, with the energy ratio providing insight into the burst composition.

major comments (2)
  1. [X-ray burst timing analysis] The recurrence time t_rec = 8196 ± 177 s is determined from only nine bursts in a 1.6-day window, despite the text noting a possible decreasing trend. This limited sample and trend indication may not establish stable clocked recurrence across the outburst, impacting the robustness of the alpha = 120-130 value used to infer pure helium bursts.
  2. [Eclipse and orbital parameter derivation] The periodic X-ray dips are interpreted as eclipses by the companion to derive P_orb, D_star,X, M2, R2, and i. While the timing is consistent, the manuscript should provide more explicit arguments or tests in this section to confirm they are not due to disk structures or other variability, as this is load-bearing for the geometric claims.
minor comments (2)
  1. The notation for asymmetric errors on the eclipse duration should be standardized throughout the text and figures.
  2. A summary table of all derived parameters would improve readability and allow easy reference.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive review and recommendation for minor revision. We address each major comment below and have revised the manuscript to strengthen the relevant sections.

read point-by-point responses
  1. Referee: The recurrence time t_rec = 8196 ± 177 s is determined from only nine bursts in a 1.6-day window, despite the text noting a possible decreasing trend. This limited sample and trend indication may not establish stable clocked recurrence across the outburst, impacting the robustness of the alpha = 120-130 value used to infer pure helium bursts.

    Authors: We agree that the sample is limited to nine bursts over 1.6 days and that a decreasing trend is noted. The reported t_rec and alpha = 120-130 are derived specifically from this interval coinciding with the NuSTAR observation; we do not claim stable clocked behavior throughout the full outburst. In revision we clarify this scope explicitly and note that the helium-burst inference applies to the observed window, with longer-term monitoring required to assess stability. revision: partial

  2. Referee: The periodic X-ray dips are interpreted as eclipses by the companion to derive P_orb, D_star,X, M2, R2, and i. While the timing is consistent, the manuscript should provide more explicit arguments or tests in this section to confirm they are not due to disk structures or other variability, as this is load-bearing for the geometric claims.

    Authors: We will expand the eclipse section with additional explicit arguments: (1) the strict periodicity matches the independently derived orbital period from optical data and burst timing; (2) the sharp, symmetric ingress/egress profiles are inconsistent with extended disk structures; (3) no analogous dip-like features appear in the persistent light curve outside eclipse phases; and (4) simultaneous optical eclipses are broader and wavelength-dependent, supporting an extended accretion-flow origin for the optical emission while the X-ray eclipse is compact. These additions address the robustness of the geometric parameters. revision: yes

Circularity Check

0 steps flagged

No circularity; all reported quantities are direct measurements or geometric derivations from observed timings

full rationale

The paper's central results consist of measured burst recurrence time t_rec from nine directly observed X-ray bursts, orbital period P_orb and eclipse duration D_star,X extracted from eclipse event timings, and companion mass/radius/inclination obtained via standard geometric relations applied to those timings. The accretion-to-thermonuclear energy ratio alpha is computed from observed persistent and burst fluences without any fitted parameter being relabeled as a prediction. No self-citations, ansatzes, or uniqueness theorems are invoked to justify load-bearing steps, and no equation reduces a claimed output to an input by construction. The noted decreasing trend in the burst subset is an observational caveat rather than a circularity issue.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The central claims rest on standard domain assumptions about the nature of type-I bursts and eclipses in LMXBs plus a small number of fitted timing parameters; no new entities are postulated.

free parameters (1)
  • burst recurrence time = 8196 ± 177 s
    Average and uncertainty fitted to a subset of nine bursts over 1.6 days
axioms (2)
  • domain assumption Periodic X-ray dips are eclipses by the companion star
    Invoked to convert eclipse duration and orbital period into mass, radius, and inclination estimates
  • domain assumption Type-I bursts are thermonuclear flashes on the neutron star surface
    Used to interpret the energy ratio as evidence for helium bursts with depleted hydrogen

pith-pipeline@v0.9.0 · 5854 in / 1600 out tokens · 76293 ms · 2026-05-16T13:01:25.827007+00:00 · methodology

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92 extracted references · 92 canonical work pages · 4 internal anchors

  1. [1]

    C., & Ransom, S

    Andersen, B. C., & Ransom, S. M. 2018, ApJL, 863, L13, doi: 10.3847/2041-8213/aad59f

  2. [2]

    2021, A&A, 654, A160, doi: 10.1051/0004-6361/202140557

    Anitra, A., Di Salvo, T., Iaria, R., et al. 2021, A&A, 654, A160, doi: 10.1051/0004-6361/202140557

  3. [3]

    2016, A&A, 586, A142, doi: 10.1051/0004-6361/201526816

    Aranzana, E., S´ anchez-Fern´ andez, C., & Kuulkers, E. 2016, A&A, 586, A142, doi: 10.1051/0004-6361/201526816

  4. [4]

    J., & Livio, M

    Armitage, P. J., & Livio, M. 1996, ApJ, 470, 1024, doi: 10.1086/177928

  5. [5]

    Arnaud, K. A. 1996, in Astronomical Society of the Pacific Conference Series, Vol. 101, Astronomical Data Analysis Software and Systems V, ed. G. H. Jacoby & J. Barnes, 17

  6. [7]

    2024, MNRAS, 529, 4311, doi: 10.1093/mnras/stae541

    Banerjee, S., & Homan, J. 2024, MNRAS, 529, 4311, doi: 10.1093/mnras/stae541

  7. [8]

    2022, ApJL, 935, L32, doi: 10.3847/2041-8213/ac87f9

    Bult, P., Altamirano, D., Arzoumanian, Z., et al. 2022, ApJL, 935, L32, doi: 10.3847/2041-8213/ac87f9

  8. [9]

    J., Luri, X., et al

    Castro-Ginard, A., McMillan, P. J., Luri, X., et al. 2021, A&A, 652, A162, doi: 10.1051/0004-6361/202039751

  9. [10]

    2025, arXiv e-prints, arXiv:2506.11966, doi: 10.48550/arXiv.2506.11966

    Cavecchi, Y., Galloway, D., Heger, A., et al. 2025, arXiv e-prints, arXiv:2506.11966, doi: 10.48550/arXiv.2506.11966

  10. [11]

    2011, MNRAS, 418, 490, doi: 10.1111/j.1365-2966.2011.19499.x

    Chakraborty, M., Bhattacharyya, S., & Mukherjee, A. 2011, MNRAS, 418, 490, doi: 10.1111/j.1365-2966.2011.19499.x

  11. [12]

    2020, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, Vol

    Chen, Y., Cui, W., Han, D., et al. 2020, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, Vol. 11444, Space Telescopes and Instrumentation 2020: Ultraviolet to Gamma Ray, ed. J.-W. A. den Herder, S. Nikzad, & K. Nakazawa, 114445B, doi: 10.1117/12.2562311

  12. [13]

    Cornelisse, R., in’t Zand, J. J. M., Verbunt, F., et al. 2003, A&A, 405, 1033, doi: 10.1051/0004-6361:20030629

  13. [14]

    Gravitational Waves. Vol. 1: The- ory and Experiments,

    Cowan, G. 1998, Statistical Data Analysis (Oxford University Press), doi: 10.1093/oso/9780198501565.001.0001

  14. [15]

    J., Hughes, A

    Cowie, F. J., Hughes, A. K., Fender, R. P., & collaboration, S. M. X.-K. 2025, The Astronomer’s Telegram, 17258, 1

  15. [16]

    D., Andrews, J

    Decleir, M., Gordon, K. D., Andrews, J. E., et al. 2022, ApJ, 930, 15, doi: 10.3847/1538-4357/ac5dbe

  16. [17]

    1991, Ap&SS, 181, 313, doi: 10.1007/BF00639097

    Demircan, O., & Kahraman, G. 1991, Ap&SS, 181, 313, doi: 10.1007/BF00639097

  17. [18]

    S., Marsh, T

    Dhillon, V. S., Marsh, T. R., Stevenson, M. J., et al. 2007, MNRAS, 378, 825, doi: 10.1111/j.1365-2966.2007.11881.x

  18. [19]

    S., Bezawada, N., Black, M., et al

    Dhillon, V. S., Bezawada, N., Black, M., et al. 2021, MNRAS, 507, 350, doi: 10.1093/mnras/stab2130 Di Salvo, T., Papitto, A., Marino, A., Iaria, R., & Burderi, L. 2023, in Handbook of X-ray and Gamma-ray Astrophysics, 147, doi: 10.1007/978-981-16-4544-0 103-1 D´ ıaz Trigo, M., & Boirin, L. 2016, Astronomische Nachrichten, 337, 368, doi: 10.1002/asna.201612315

  19. [20]

    2025, PASJ, 77, L17, doi: 10.1093/pasj/psae117

    Dohi, A., Nishimura, N., Hirai, R., et al. 2025, PASJ, 77, L17, doi: 10.1093/pasj/psae117

  20. [21]

    2024, arXiv e-prints, arXiv:2403.03127, doi: 10.48550/arXiv.2403.03127

    Doroshenko, V. 2024, arXiv e-prints, arXiv:2403.03127, doi: 10.48550/arXiv.2403.03127

  21. [22]

    2024, A&A, 685, A82, doi: 10.1051/0004-6361/202347628

    Edenhofer, G., Zucker, C., Frank, P., et al. 2024, A&A, 685, A82, doi: 10.1051/0004-6361/202347628

  22. [23]

    Eggleton, P. P. 1983, ApJ, 268, 368, doi: 10.1086/160960

  23. [24]

    2019, ApJ, 887, 30, doi: 10.3847/1538-4357/ab4d59

    Fiocchi, M., Bazzano, A., Bruni, G., et al. 2019, ApJ, 887, 30, doi: 10.3847/1538-4357/ab4d59

  24. [25]

    Clayton, G. C. 2019, ApJ, 886, 108, doi: 10.3847/1538-4357/ab4c3a

  25. [26]

    Y., Hanawa, T., & Miyaji, S

    Fujimoto, M. Y., Hanawa, T., & Miyaji, S. 1981, ApJ, 247, 267, doi: 10.1086/159034

  26. [27]

    K., Johnston, Z., Goodwin, A., & He, C.-C

    Galloway, D. K., Johnston, Z., Goodwin, A., & He, C.-C. 2022, ApJS, 263, 30, doi: 10.3847/1538-4365/ac98c9

  27. [28]

    K., & Keek, L

    Galloway, D. K., & Keek, L. 2021, in Astrophysics and Space Science Library, Vol. 461, Timing Neutron Stars:

  28. [29]

    M´ endez, & C

    Belloni, M. M´ endez, & C. Zhang, 209–262, doi: 10.1007/978-3-662-62110-3 5

  29. [30]

    K., in’t Zand, J., Chenevez, J., et al

    Galloway, D. K., in’t Zand, J., Chenevez, J., et al. 2020, ApJS, 249, 32, doi: 10.3847/1538-4365/ab9f2e

  30. [31]

    F., Iaria, R., Di Salvo, T., et al

    Gambino, A. F., Iaria, R., Di Salvo, T., et al. 2019, A&A, 625, A92, doi: 10.1051/0004-6361/201832984 Garc´ ıa, J., Dauser, T., Lohfink, A., et al. 2014, ApJ, 782, 76, doi: 10.1088/0004-637X/782/2/76

  31. [32]

    2024, The Journal of Open Source Software, 9, 7023, doi: 10.21105/joss.07023

    Gordon, K. 2024, The Journal of Open Source Software, 9, 7023, doi: 10.21105/joss.07023

  32. [33]

    D., Cartledge, S., & Clayton, G

    Gordon, K. D., Cartledge, S., & Clayton, G. C. 2009, ApJ, 705, 1320, doi: 10.1088/0004-637X/705/2/1320

  33. [34]

    D., Clayton, G

    Gordon, K. D., Clayton, G. C., Decleir, M., et al. 2023, ApJ, 950, 86, doi: 10.3847/1538-4357/accb59

  34. [35]

    D., Misselt, K

    Gordon, K. D., Misselt, K. A., Bouwman, J., et al. 2021, ApJ, 916, 33, doi: 10.3847/1538-4357/ac00b7

  35. [36]

    2025, The Astronomer’s Telegram, 17272, 1

    Guillot, S., Xin, L., Marino, A., Coti Zelati, F., & Rea, N. 2025, The Astronomer’s Telegram, 17272, 1

  36. [37]

    A., Craig, W

    Harrison, F. A., Craig, W. W., Christensen, F. E., et al. 2013, ApJ, 770, 103, doi: 10.1088/0004-637X/770/2/103

  37. [38]

    Hastings, W. K. 1970, Biometrika, 57, 97, doi: 10.1093/biomet/57.1.97

  38. [39]

    Hunter, J. D. 2007, Computing in Science and Engineering, 9, 90, doi: 10.1109/MCSE.2007.55 EP J171159.4−333253: a rare clocked burster with eclipses27

  39. [40]

    2024, A&A, 691, A189, doi: 10.1051/0004-6361/202451703

    Illiano, G., Papitto, A., Marino, A., et al. 2024, A&A, 691, A189, doi: 10.1051/0004-6361/202451703

  40. [41]

    K., & Ammon, K

    Jordi, K., Grebel, E. K., & Ammon, K. 2006, A&A, 460, 339, doi: 10.1051/0004-6361:20066082

  41. [42]

    C., & Rappaport, S

    Joss, P. C., & Rappaport, S. A. 1984, ARA&A, 22, 537, doi: 10.1146/annurev.aa.22.090184.002541

  42. [43]

    S., & Bleeker, J

    Kaastra, J. S., & Bleeker, J. A. M. 2016, A&A, 587, A151, doi: 10.1051/0004-6361/201527395

  43. [44]

    Kajava, J. J. E., Motta, S. E., Sanna, A., et al. 2019, MNRAS, 488, L18, doi: 10.1093/mnrasl/slz089

  44. [45]

    R., & Wijnands, R

    King, A. R., & Wijnands, R. 2006, MNRAS, 366, L31, doi: 10.1111/j.1745-3933.2005.00126.x

  45. [46]

    Kong, A. K. H., Aryan, A., Li, K. L., et al. 2025, The Astronomer’s Telegram, 17280, 1

  46. [47]

    2025, MNRAS, 540, 2305, doi: 10.1093/mnras/staf853

    Kormpakis, T., Linares, M., & Jos´ e, J. 2025, MNRAS, 540, 2305, doi: 10.1093/mnras/staf853

  47. [48]

    Kuulkers, E., in’t Zand, J. J. M., Cornelisse, R., et al. 2000, A&A, 358, 993, doi: 10.48550/arXiv.astro-ph/0004275

  48. [49]

    2013, A&A, 552, A32, doi: 10.1051/0004-6361/201219447 La Monaca, F., Di Marco, A., Coti Zelati, F., et al

    Kuulkers, E., Kouveliotou, C., Belloni, T., et al. 2013, A&A, 552, A32, doi: 10.1051/0004-6361/201219447 La Monaca, F., Di Marco, A., Coti Zelati, F., et al. 2025, A&A, 702, A101, doi: 10.1051/0004-6361/202555134

  49. [50]

    Lewin, W. H. G., van Paradijs, J., & Taam, R. E. 1993, SSRv, 62, 223, doi: 10.1007/BF00196124

  50. [51]

    Lewin, W. H. G., van Paradijs, J., & van den Heuvel, E. P. J., eds. 1995, X-ray binaries

  51. [52]

    A., & Homan, J

    Lin, D., Remillard, R. A., & Homan, J. 2007, ApJ, 667, 1073, doi: 10.1086/521181

  52. [53]

    Ludlam, R. M. 2024, Ap&SS, 369, 16, doi: 10.1007/s10509-024-04281-y

  53. [54]

    2021, ApJ, 911, 45, doi: 10.3847/1538-4357/abe62f

    Luo, J., Ransom, S., Demorest, P., et al. 2021, ApJ, 911, 45, doi: 10.3847/1538-4357/abe62f

  54. [55]

    2025, A&A, 699, A288, doi: 10.1051/0004-6361/202554075

    Malacaria, C., Papitto, A., Campana, S., et al. 2025, A&A, 699, A288, doi: 10.1051/0004-6361/202554075

  55. [56]

    2019, MNRAS, 490, 2300, doi: 10.1093/mnras/stz2726

    Marino, A., Del Santo, M., Cocchi, M., et al. 2019, MNRAS, 490, 2300, doi: 10.1093/mnras/stz2726

  56. [57]

    M., et al

    Marino, A., Anitra, A., Mazzola, S. M., et al. 2022, MNRAS, 515, 3838, doi: 10.1093/mnras/stac2038

  57. [58]

    D., Del Santo, M., et al

    Marino, A., Russell, T. D., Del Santo, M., et al. 2023, MNRAS, 525, 2366, doi: 10.1093/mnras/stad2386

  58. [59]

    Aql X-1 from dawn 'til dusk: the early rise, fast state transition and decay of its 2024 outburst

    Marino, A., Coti Zelati, F., Alabarta, K., et al. 2025b, arXiv e-prints, arXiv:2511.16437, doi: 10.48550/arXiv.2511.16437

  59. [60]

    P., Parsons, S

    McAllister, M., Littlefair, S. P., Parsons, S. G., et al. 2019, MNRAS, 486, 5535, doi: 10.1093/mnras/stz976

  60. [61]

    V., Lutovinov, A

    Molkov, S. V., Lutovinov, A. A., Tsygankov, S. S., et al. 2024, A&A, 690, A353, doi: 10.1051/0004-6361/202450581

  61. [62]

    S., Dewangan, G

    Mondal, A. S., Dewangan, G. C., & Raychaudhuri, B. 2020, MNRAS, 494, 3177, doi: 10.1093/mnras/staa1001

  62. [63]

    Courvoisier, T. J.-L. 1987, ApJ, 313, 792, doi: 10.1086/165017

  63. [64]

    2011, MNRAS, 418, 490, doi: 10.1111/j.1365-2966.2011.19499.x

    Motta, S., D’A` ı, A., Papitto, A., et al. 2011, MNRAS, 414, 1508, doi: 10.1111/j.1365-2966.2011.18483.x Mu˜ noz-Darias, T., Fender, R. P., Motta, S. E., & Belloni, T. M. 2014, MNRAS, 443, 3270, doi: 10.1093/mnras/stu1334

  64. [65]

    P., Lu, J

    Muno, M. P., Lu, J. R., Baganoff, F. K., et al. 2005, ApJ, 633, 228, doi: 10.1086/444586 Nasa High Energy Astrophysics Science Archive Research Center (Heasarc). 2014, HEAsoft: Unified Release of FTOOLS and XANADU,, Astrophysics Source Code Library, record ascl:1408.004

  65. [66]

    S., Sanna, A., et al

    Ng, M., Ray, P. S., Sanna, A., et al. 2024, ApJL, 968, L7, doi: 10.3847/2041-8213/ad4edb

  66. [67]

    R., Wu, J

    Ni, K. R., Wu, J. H., Wen, W. F., & Yuan, W. 2025, The Astronomer’s Telegram, 17247, 1

  67. [68]

    A., Wolf, C., Bessell, M

    Onken, C. A., Wolf, C., Bessell, M. S., et al. 2024, PASA, 41, e061, doi: 10.1017/pasa.2024.53

  68. [69]

    2024, A&A, 682, A19, doi: 10.1051/0004-6361/202347955

    Panizo-Espinar, G., Mu˜ noz-Darias, T., Armas Padilla, M., et al. 2024, A&A, 682, A19, doi: 10.1051/0004-6361/202347955

  69. [70]

    2025, A&A, 694, A37, doi: 10.1051/0004-6361/202451775

    Papitto, A., Di Marco, A., Poutanen, J., et al. 2025, A&A, 694, A37, doi: 10.1051/0004-6361/202451775

  70. [71]

    J., & Mamajek, E

    Pecaut, M. J., & Mamajek, E. E. 2013, ApJS, 208, 9, doi: 10.1088/0067-0049/208/1/9

  71. [72]

    2018, MNRAS, 479, 4084, doi: 10.1093/mnras/sty1735 Planck Collaboration, Aghanim, N., Ashdown, M., et al

    Pintore, F., Sanna, A., Riggio, A., et al. 2018, MNRAS, 479, 4084, doi: 10.1093/mnras/sty1735 Planck Collaboration, Aghanim, N., Ashdown, M., et al. 2016, A&A, 596, A109, doi: 10.1051/0004-6361/201629022

  72. [73]

    2011, PRESTO: PulsaR Exploration and Search TOolkit,, Astrophysics Source Code Library, record ascl:1107.017 http://ascl.net/1107.017

    Ransom, S. 2011, PRESTO: PulsaR Exploration and Search TOolkit,, Astrophysics Source Code Library, record ascl:1107.017 http://ascl.net/1107.017

  73. [74]

    Ransom, S. M. 2001, PhD thesis, Harvard University, Massachusetts

  74. [75]

    M., Eikenberry, S

    Ransom, S. M., Eikenberry, S. S., & Middleditch, J. 2002, AJ, 124, 1788, doi: 10.1086/342285

  75. [76]

    2025, MNRAS, 544, 13, doi: 10.1093/mnras/staf1611

    Rikame, K., Paul, B., Sharma, R., & Jithesh, V. 2025, MNRAS, 544, 13, doi: 10.1093/mnras/staf1611

  76. [77]

    D., Norris, J

    Scargle, J. D., Norris, J. P., Jackson, B., & Chiang, J. 2013, ApJ, 764, 167, doi: 10.1088/0004-637X/764/2/167

  77. [78]

    A., & Dhillon, V

    Smith, D. A., & Dhillon, V. S. 1998, MNRAS, 301, 767, doi: 10.1046/j.1365-8711.1998.02065.x

  78. [79]

    L., Archibald, A

    Susobhanan, A., Kaplan, D. L., Archibald, A. M., et al. 2024, ApJ, 971, 150, doi: 10.3847/1538-4357/ad59f7 28W ang et al

  79. [80]

    Smale, A. P. 1993, ApJ, 408, 651, doi: 10.1086/172624

  80. [81]

    1999, ApJL, 514, L27, doi: 10.1086/311933

    Ubertini, P., Bazzano, A., Cocchi, M., et al. 1999, ApJL, 514, L27, doi: 10.1086/311933

Showing first 80 references.