REVIEW 1 major objections 4 minor 2 cited by
Bridging the Gap: OPTICAM Reveals the Hidden Spin of the WZ Sge Star GOTO 065054.49+593624.51
T0 review · 1 major / 4 minor · reviewed 2026-08-10 · deepseek-v4-flash
Pith's one-line read A 148-second pulse reveals a hidden white-dwarf spin in a WZ Sge star.
desk verdict A well-analyzed single-epoch periodicity that is likely real; the spin interpretation is plausible but unproven, and the magnetic field argument has a fixable inconsistency. 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 detection rests on Lomb-Scargle periodograms with a Vaughan (2005) noise model for confidence thresholds, bootstrap resampling for the frequency uncertainty and coherence (Q factor from a Lorentzian fit), and phase folding of the epoch-4 light curves. The physical argument is that a blue, coherent, ~148 s modulation appearing only when the disc fades between outburst phases matches the signature of magnetically channeled accretion onto a spinning white dwarf, as seen in intermediate polars.
What would settle it
A high-cadence observation of GOTO 0650 in quiescence that does not show a ~148 second modulation in g-band would weaken the spin interpretation, as would finding the periodicity in a band or epoch where the accretion geometry is unchanged but the disc is dominant. The authors explicitly say quiescent observations are required to test this hypothesis.
Extended reading notes
Core claim
Using high-cadence g, r, i photometry with OPTICAM over five nights across a factor of ~100 in brightness, the authors find a statistically significant signal at 148.2 s (6.73 mHz) in the g-band of epoch 4, with a false alarm probability of 1.16e-6 and a Q factor of 3422, indicating a highly coherent oscillation. The signal has a peak-to-peak amplitude of about 10% in g-band, weakens toward redder bands, and is absent in comparison stars and local background, ruling out instrumental artifacts. The authors interpret it as the spin period of the accreting white dwarf, argue that dwarf nova oscillations, non-radial pulsations, and precessing inner disc QPOs are unlikely on timescale and temperature grounds, and estimate a magnetic field of order $10^{4}$ G. They explicitly state that quiescent observations are required to confirm the spin interpretation.
Load-bearing premise
The assumption that the 148-second pulse is the rotating accretion spot of the white dwarf rather than a disc oscillation, a stellar pulsation, or a precessing inner disc; the paper argues against these alternatives but has no direct proof of the spin link.
Editorial extensions
If this is right
- GOTO 0650 becomes the second WZ Sge-type star, after WZ Sge itself, with a candidate white-dwarf spin period, and the first detected while the system is still in outburst.
- The 148 s period sits between the spin periods of CC Scl and V455 And, filling the gap between slow and fast rotating magnetic white dwarfs below the period gap.
- The implied magnetic field of about 10^4 G strengthens the view that even weak magnetic fields shape the behaviour of WZ Sge stars.
Reading between the lines
- If the spin interpretation is correct, the same modulation should reappear in quiescent observations with a stable phase; the authors explicitly call for this test.
- The restriction of the signal to the dip between the main outburst and rebrightenings implies a dramatic change in accretion geometry across the outburst cycle; a testable prediction is that the modulation amplitude tracks the system's position in the cycle.
- The g-band, dip-only detection suggests a practical recipe for hunting hidden spins in other WZ Sge stars: high-cadence multi-band monitoring during the faint dip phase rather than at outburst peak.
- If confirmed, the combination of the spin period and the ~91 min superhump period would place GOTO 0650 in a regime where magnetic torques could measurably influence the disc's inner radius, which a future timing campaign could check.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This paper presents high-cadence OPTICAM photometry of the WZ Sge-type dwarf nova GOTO 065054.49+593624.51 during the decline and dip following its 2024 superoutburst. A coherent periodicity at P_omega ~ 148.2 s is detected in the g-band light curve of epoch 4 with a false alarm probability of 1.16e-6 and a trials-corrected global significance of 0.0016 per cent. The authors interpret the signal as the spin period of the accreting white dwarf, discuss alternative origins (DNOs, non-radial pulsations, QPOs), and use magnetospheric arguments to argue that the observed period is the fundamental spin period rather than its first harmonic. If confirmed, the system would bridge the gap between intermediate- and fast-rotating intermediate polars below the period gap.
Significance. The reported detection is statistically well supported: the analysis includes bootstrap frequency uncertainties, a Lorentzian fit with Q ~ 3422, comparison with background and reference stars, and simulations for confidence thresholds. The identification of a candidate spin period in a WZ Sge system during the dip phase is of genuine interest, as it directly probes magnetospheric accretion in the lowest-mass-transfer-rate CVs. The paper also gives a reasonable discussion of alternative interpretations. However, the spin-period identification is not unique: the observed period could be the first harmonic of a longer spin period, and the magnetic-field argument used to rule out this possibility contains an internal inconsistency (see Major Comment 1). The significance of the result therefore depends on resolving this ambiguity; as it stands, the conclusion is a plausible but not fully supported hypothesis.
major comments (1)
- [Section 4, magnetic-field estimates] The magnetic-field argument meant to break the spin/harmonic degeneracy is internally inconsistent. On one hand, the authors derive a lower limit of B ~ 2e4 G from requiring r_M >= R_WD at Mdot ~ 1e-10 Msun/yr and an upper limit of B <~ 4e4 G from the outburst state. On the other hand, the equilibrium estimates give B ~ 5e4 G for P_spin = 148.5 s and B ~ 1e5 G for P_spin = 297 s; both exceed the derived upper limit, and the concluding 'B ~ 1e4 G' falls below the stated lower limit. The additional argument that the 1e5 G case would require a super-Eddington mass accretion rate does not exclude the 5e4 G case, which is also outside the allowed range. Consequently, the harmonic ambiguity is not resolved by this reasoning, and the identification of 148.5 s as the fundamental spin period, and the associated 'bridge the gap' claim, remain unsupported by the magnetic-field argument as written.
minor comments (4)
- [Abstract] The word 'rebrigthenings' should be 'rebrightenings'.
- [Section 3, paragraph 2] The sentence 'We are not able to recover any signal from the LSP but, despite this, the g-band lightcurve from that same epoch exhibits short-term flares qualitatively similar to those observed in epoch 4' lacks a clear referent; it should specify that the LSP refers to epoch 5.
- [Section 4] The notation 'for P_omega = 1 and 2xP_spin' is ambiguous and should be rewritten to clarify the two cases, e.g., 'for P_spin = P_omega and P_spin = 2P_omega'.
- [Section 4] The phrase 'The same is not true for Epoch 2' is confusing; the authors should clarify that the disc is closer to a stationary configuration in Epoch 2 than in Epoch 3, which enables the upper-limit argument.
Circularity Check
No significant circularity: the 148.2 s periodicity is measured directly from the light curve, and the spin interpretation is an explicitly hypotheses-driven inference rather than a construction from fitted inputs.
full rationale
The central detection of P_omega = 148.2 s is obtained directly from the Lomb-Scargle periodogram of the epoch-4 g-band light curve, with confidence levels set by white-noise simulations and the signal checked against reference stars and background. The period is not produced by a model fitted to the data, and no equation in the paper defines the detected period in terms of the spin hypothesis or vice versa. The spin-period interpretation is an astrophysical inference supported by timescale, color, and comparison arguments, and the authors explicitly state that quiescent observations are required to test it. The magnetic-field estimates are used only to argue that the detected period is the fundamental rather than a harmonic; these estimates are acknowledged as highly uncertain and do not feed back into the period measurement. Self-citations, including the OPTICAM instrument papers, the Tampo (2024) superhump report, and Veresvarska et al. (2024), are contextual and are not load-bearing for the central periodicity claim. The internal inconsistency in the B-field limits noted by a skeptical reader is a scientific/correctness concern about the harmonic ambiguity, not a circularity in the derivation chain.
Assumptions & free parameters
free parameters (2)
- Mass accretion rate during epoch 4 =
~1e-10 Msun/yr
- White dwarf mass =
0.8 Msun
assumptions (3)
- domain assumption GOTO 0650 is a WZ Sge-type dwarf nova with the reported outburst classification
- domain assumption Accretion luminosity scales linearly with mass accretion rate (L ∝ Mdot)
- domain assumption Ghosh and Lamb magnetospheric radius and co-rotation relations apply
Cite this review
Pith. "Pith review of Bridging the Gap: OPTICAM Reveals the Hidden Spin of the WZ Sge Star GOTO 065054.49+593624.51." pith.science (2026). https://pith.science/paper/NTQURZDP
@misc{pith2026250111669,
author = {Pith},
title = {Pith review of: Bridging the Gap: OPTICAM Reveals the Hidden Spin of the WZ Sge Star GOTO 065054.49+593624.51},
year = {2026},
howpublished = {\url{https://pith.science/paper/NTQURZDP}},
note = {Machine review of arXiv:2501.11669}
}
abstract
WZ Sge stars are highly evolved accreting white dwarf systems (AWDs) exhibiting remarkably large amplitude outbursts (a.k.a. super-outbursts), typically followed by short rebrightenings/echo outbursts. These systems have some of the lowest mass transfer rates among AWDs, making even low magnetic fields dynamically important. Such magnetic fields are often invoked to explain the phenomenology observed in these systems, such as their X-ray luminosity and long periods of quiescence (30+ years). However, the detection of these is very elusive given the quenching of the accretion columns during outburst and the low luminosity of these systems during quiescence. Here we present high-cadence multi-band observations with {\it OPTICAM} of the recent outburst of the recently discovered WZ Sge star GOTO065054.49+593624.51, during the end of the main outburst and the dip in-between rebrightenings, covering 2 orders of magnitude in brightness. Our observations reveal the presence of a statistically significant signal with $P_{\omega}\simeq148$ seconds in the bluer ($g$) band which is detected only during the dip between the main outburst and the rebrigthenings. We interpret this signal as the spin period of the AWD. If confirmed, GOTO 0650 would bridge the gap between intermediate- and fast-rotating intermediate polars (IPs) below the period gap.
Figures
Figures from the paper (2 more)
Forward citations
Cited by 2 Pith papers
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phoptic -- a Python package for reducing astronomical images
phoptic provides a single open-source Python pipeline that reduces images from OPTICAM, ULTRACAM, HiPERCAM, and MEXMAN into photometric light curves.
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GOTO065054+593624: a 8.5 mag amplitude dwarf nova identified in real time via Kilonova Seekers
GOTO0650 is a WZ Sge-type dwarf nova with an 8.5 magnitude outburst, ten echo outbursts, and properties consistent with a candidate period bouncer.
Reference graph
Works this paper leans on
-
[1]
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-
[2]
thebibliography @urlcharsother \@makeother \ & \# \^ \_ \ @doi @urlcharsother \@ifnextchar [ @doi@ @doi@[] @doi@[#1]#2 \@tempa #1 \@tempa\@empty http://dx.doi.org/#2 doi:#2 http://dx.doi.org/#2 #1 @eprint#1#2 @eprint@#1:#2::\@nil @eprint@arXiv#1 http://arxiv.org/abs/#1 arXiv:#1 @eprint@dblp#1 http://dblp.uni-trier.de/rec/bibtex/#1.xml dblp:#1 @eprint@#1:#...
-
[3]
Araujo-Betancor S., et al., 2005, @doi [ ] 10.1051/0004-6361:20041736 , https://ui.adsabs.harvard.edu/abs/2005A&A...430..629A 430, 629
-
[4]
Bellm E. C., et al., 2019a, @doi [ ] 10.1088/1538-3873/aaecbe , https://ui.adsabs.harvard.edu/abs/2019PASP..131a8002B 131, 018002
-
[5]
Bellm E. C., et al., 2019b, @doi [ ] 10.1088/1538-3873/ab0c2a , https://ui.adsabs.harvard.edu/abs/2019PASP..131f8003B 131, 068003
-
[6]
Belloni T., Psaltis D., van der Klis M., 2002, @doi [ ] 10.1086/340290 , https://ui.adsabs.harvard.edu/abs/2002ApJ...572..392B 572, 392
doi:10.1086/340290 2002
-
[7]
Bhattacharya S., Bhattacharyya S., 2024, The Astronomer's Telegram, https://ui.adsabs.harvard.edu/abs/2024ATel16866....1B 16866, 1
work page 2024
-
[8]
Bloemen S., Steeghs D., De Smedt K., Vos J., G \"a nsicke B. T., Marsh T. R., Rodriguez-Gil P., 2013, @doi [ ] 10.1093/mnras/sts622 , https://ui.adsabs.harvard.edu/abs/2013MNRAS.429.3433B 429, 3433
Show all 62 references
-
[9]
Bradley L., et al., 2024, astropy/photutils: 1.13.0, @doi 10.5281/zenodo.12585239 , https://doi.org/10.5281/zenodo.12585239
2024 doi
-
[10]
Campana S., Stella L., Mereghetti S., de Martino D., 2018, @doi [ ] 10.1051/0004-6361/201730769 , https://ui.adsabs.harvard.edu/abs/2018A&A...610A..46C 610, A46
2018 doi
-
[11]
Castro Segura N., et al., 2021, @doi [ ] 10.1093/mnras/staa2516 , https://ui.adsabs.harvard.edu/abs/2021MNRAS.501.1951C 501, 1951
2021 doi
-
[12]
Castro A., et al., 2019, @doi [ ] 10.22201/ia.01851101p.2019.55.02.20 , https://ui.adsabs.harvard.edu/abs/2019RMxAA..55..363C 55, 363
2019 doi
-
[13]
Castro A., et al., 2024, @doi [ ] 10.1016/j.newast.2024.102262 , https://ui.adsabs.harvard.edu/abs/2024NewA..11202262C 112, 102262
2024
-
[14]
C., 1993, @doi [Baltic Astronomy] 10.1515/astro-1993-3-410 , https://ui.adsabs.harvard.edu/abs/1993BaltA...2..407C 2, 407
Clemens J. C., 1993, @doi [Baltic Astronomy] 10.1515/astro-1993-3-410 , https://ui.adsabs.harvard.edu/abs/1993BaltA...2..407C 2, 407
1993 doi
-
[15]
J., et al., 2024, in Marshall H
Dyer M. J., et al., 2024, in Marshall H. K., Spyromilio J., Usuda T., eds, Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series Vol. 13094, Ground-based and Airborne Telescopes X. p. 130941X ( @eprint arXiv 2407.17176 ), @doi 10.1117/12.3018305
2024 arXiv
-
[16]
Eracleous M., Horne K., 1996, @doi [ ] 10.1086/177979 , https://ui.adsabs.harvard.edu/abs/1996ApJ...471..427E 471, 427
1996 doi
-
[17]
S., 2022, @doi [ ] 10.1093/mnras/stac116 , https://ui.adsabs.harvard.edu/abs/2022MNRAS.511.5385G 511, 5385
Georganti M., Knigge C., Castro Segura N., Long K. S., 2022, @doi [ ] 10.1093/mnras/stac116 , https://ui.adsabs.harvard.edu/abs/2022MNRAS.511.5385G 511, 5385
2022 doi
-
[18]
K., 1979, @doi [ ] 10.1086/157498 , https://ui.adsabs.harvard.edu/abs/1979ApJ...234..296G 234, 296
Ghosh P., Lamb F. K., 1979, @doi [ ] 10.1086/157498 , https://ui.adsabs.harvard.edu/abs/1979ApJ...234..296G 234, 296
1979 doi
-
[19]
M., 2020, @doi [Advances in Space Research] 10.1016/j.asr.2019.10.022 , https://ui.adsabs.harvard.edu/abs/2020AdSpR..66.1004H 66, 1004
Hameury J. M., 2020, @doi [Advances in Space Research] 10.1016/j.asr.2019.10.022 , https://ui.adsabs.harvard.edu/abs/2020AdSpR..66.1004H 66, 1004
2020 doi
-
[20]
J., VanderPlas J
Ivezi \'c Z ., Connolly A. J., VanderPlas J. T., Gray A., 2014, Statistics, Data Mining, and Machine Learning in Astronomy: A Practical Python Guide for the Analysis of Survey Data , @doi 10.1515/9781400848911
2014 doi
-
[21]
Kato T., 2015, @doi [ ] 10.1093/pasj/psv077 , https://ui.adsabs.harvard.edu/abs/2015PASJ...67..108K 67, 108
2015 doi
-
[22]
Killestein T., et al., 2024a, The Astronomer's Telegram, https://ui.adsabs.harvard.edu/abs/2024ATel16842....1K 16842, 1
-
[23]
Killestein T., et al., 2024b, The Astronomer's Telegram, https://ui.adsabs.harvard.edu/abs/2024ATel16858....1K 16858, 1
- [24]
-
[25]
Kimura M., et al., 2018, @doi [ ] 10.1093/pasj/psy037 , https://ui.adsabs.harvard.edu/abs/2018PASJ...70...47K 70, 47
2018 doi
-
[26]
Kimura M., Osaki Y., Kato T., Mineshige S., 2020, @doi [ ] 10.1093/pasj/psz144 , https://ui.adsabs.harvard.edu/abs/2020PASJ..tmp..156K
2020 doi
-
[27]
I., Steeghs D., Long K
Knigge C., Hynes R. I., Steeghs D., Long K. S., Araujo-Betancor S., Marsh T. R., 2002, @doi [ ] 10.1086/345591 , https://ui.adsabs.harvard.edu/abs/2002ApJ...580L.151K 580, L151
2002 doi
-
[28]
Knigge C., Baraffe I., Patterson J., 2011, @doi [ ] 10.1088/0067-0049/194/2/28 , https://ui.adsabs.harvard.edu/abs/2011ApJS..194...28K 194, 28
2011 doi
-
[29]
Lasota J.-P., 2016, Black Hole Accretion Discs . p. 1, @doi 10.1007/978-3-662-52859-4_1
2016 doi
-
[30]
R., I kiewicz K., Mason P
Littlefield C., Scaringi S., Garnavich P., Szkody P., Kennedy M. R., I kiewicz K., Mason P. A., 2021, @doi [ ] 10.3847/1538-3881/ac062b , https://ui.adsabs.harvard.edu/abs/2021AJ....162...49L 162, 49
2021 doi
-
[31]
R., 1976, @doi [ ] 10.1007/BF00648343 , https://ui.adsabs.harvard.edu/abs/1976Ap&SS..39..447L 39, 447
Lomb N. R., 1976, @doi [ ] 10.1007/BF00648343 , https://ui.adsabs.harvard.edu/abs/1976Ap&SS..39..447L 39, 447
1976 doi
-
[32]
M., Lovelace R
Long M., Romanova M. M., Lovelace R. V. E., 2005, @doi [ ] 10.1086/497000 , https://ui.adsabs.harvard.edu/abs/2005ApJ...634.1214L 634, 1214
2005 doi
-
[33]
A., Han Z., 2013, @doi [ ] 10.1088/2041-8205/778/2/L32 , https://ui.adsabs.harvard.edu/abs/2013ApJ...778L..32M 778, L32
Ma X., Chen X., Chen H.-l., Denissenkov P. A., Han Z., 2013, @doi [ ] 10.1088/2041-8205/778/2/L32 , https://ui.adsabs.harvard.edu/abs/2013ApJ...778L..32M 778, L32
2013 doi
-
[35]
McCully C., et al., 2018, astropy/astroscrappy: v1.0.5 Zenodo Release , @doi 10.5281/zenodo.1482019
2018 doi
-
[36]
Naylor T., 1998, @doi [ ] 10.1046/j.1365-8711.1998.01314.x , https://ui.adsabs.harvard.edu/abs/1998MNRAS.296..339N 296, 339
1998
-
[37]
A., et al., 2024, @doi [ ] 10.1093/mnrasl/slae035 , https://ui.adsabs.harvard.edu/abs/2024MNRAS.531L..82P 531, L82
Paice J. A., et al., 2024, @doi [ ] 10.1093/mnrasl/slae035 , https://ui.adsabs.harvard.edu/abs/2024MNRAS.531L..82P 531, L82
2024 doi
-
[38]
F., et al., 2017, @doi [ ] 10.1093/mnras/stw3293 , https://ui.adsabs.harvard.edu/abs/2017MNRAS.466.2855P 466, 2855
Pala A. F., et al., 2017, @doi [ ] 10.1093/mnras/stw3293 , https://ui.adsabs.harvard.edu/abs/2017MNRAS.466.2855P 466, 2855
2017 doi
-
[39]
Patterson J., 1980, @doi [ ] 10.1086/158336 , https://ui.adsabs.harvard.edu/abs/1980ApJ...241..235P 241, 235
1980 doi
-
[40]
Patterson J., 2011, @doi [ ] 10.1111/j.1365-2966.2010.17881.x , https://ui.adsabs.harvard.edu/abs/2011MNRAS.411.2695P 411, 2695
2011
-
[41]
Patterson J., Richman H., Kemp J., Mukai K., 1998, @doi [ ] 10.1086/316152 , https://ui.adsabs.harvard.edu/abs/1998PASP..110..403P 110, 403
1998 doi
-
[42]
Patterson J., et al., 2005, @doi [ ] 10.1086/447771 , https://ui.adsabs.harvard.edu/abs/2005PASP..117.1204P 117, 1204
2005 doi
- [43]
-
[44]
L., Nather R
Robinson E. L., Nather R. E., Patterson J., 1978, @doi [ ] 10.1086/155766 , https://ui.adsabs.harvard.edu/abs/1978ApJ...219..168R 219, 168
1978 doi
-
[45]
D., 1982, @doi [ ] 10.1086/160554 , https://ui.adsabs.harvard.edu/abs/1982ApJ...263..835S 263, 835
Scargle J. D., 1982, @doi [ ] 10.1086/160554 , https://ui.adsabs.harvard.edu/abs/1982ApJ...263..835S 263, 835
1982 doi
-
[46]
F., Wood J
Skidmore W., Welsh W. F., Wood J. H., Catal \'a n M. S., Horne K., 1999, @doi [ ] 10.1046/j.1365-8711.1999.03003.x , https://ui.adsabs.harvard.edu/abs/1999MNRAS.310..750S 310, 750
1999
-
[47]
Smak J., 1993, , https://ui.adsabs.harvard.edu/abs/1993AcA....43..101S 43, 101
1993
- [48]
-
[49]
T., Marsh T
Southworth J., G \"a nsicke B. T., Marsh T. R., de Martino D., Hakala P., Littlefair S., Rodr \' guez-Gil P., Szkody P., 2006, @doi [ ] 10.1111/j.1365-2966.2006.11042.x , https://ui.adsabs.harvard.edu/abs/2006MNRAS.373..687S 373, 687
2006
-
[50]
Steeghs D., et al., 2022, @doi [ ] 10.1093/mnras/stac013 , https://ui.adsabs.harvard.edu/abs/2022MNRAS.511.2405S 511, 2405
2022 doi
-
[51]
Szkody P., 2021, @doi [Frontiers in Astronomy and Space Sciences] 10.3389/fspas.2021.759686 , https://ui.adsabs.harvard.edu/abs/2021FrASS...8..184S 8, 184
2021
-
[52]
Tampo Y., 2024, GOTO065054.49+593624.51: type-E rebrightening WZ Sge star?, http://ooruri.kusastro.kyoto-u.ac.jp/mailman3/hyperkitty/list/vsnet-alert@ooruri.kusastro.kyoto-u.ac.jp/thread/TWMZC3AKMJHBRPUBNRLYHGTKDCJKITDQ/
2024
-
[53]
Toloza O., et al., 2016, @doi [ ] 10.1093/mnras/stw838 , https://ui.adsabs.harvard.edu/abs/2016MNRAS.459.3929T 459, 3929
2016 doi
-
[55]
T., 2018b, @doi [ ] 10.3847/1538-4365/aab766 , https://ui.adsabs.harvard.edu/abs/2018ApJS..236...16V 236, 16
VanderPlas J. T., 2018b, @doi [ ] 10.3847/1538-4365/aab766 , https://ui.adsabs.harvard.edu/abs/2018ApJS..236...16V 236, 16
-
[56]
Vaughan S., 2005, @doi [ ] 10.1051/0004-6361:20041453 , https://ui.adsabs.harvard.edu/abs/2005A&A...431..391V 431, 391
2005 doi
-
[57]
S., Uttley P., 2003, @doi [ ] 10.1046/j.1365-2966.2003.07042.x , https://ui.adsabs.harvard.edu/abs/2003MNRAS.345.1271V 345, 1271
Vaughan S., Edelson R., Warwick R. S., Uttley P., 2003, @doi [ ] 10.1046/j.1365-2966.2003.07042.x , https://ui.adsabs.harvard.edu/abs/2003MNRAS.345.1271V 345, 1271
2003
-
[58]
Veresvarska M., et al., 2024, @doi [ ] 10.1093/mnras/stae2279 , https://ui.adsabs.harvard.edu/abs/2024MNRAS.534.3087V 534, 3087
2024 doi
-
[59]
Warner B., 1987, @doi [ ] 10.1093/mnras/227.1.23 , https://ui.adsabs.harvard.edu/abs/1987MNRAS.227...23W 227, 23
1987 doi
-
[60]
Warner B., 1995, Cataclysmic variable stars . Vol. 28
1995
-
[61]
A., Warner B., 2002, @doi [ ] 10.1046/j.1365-8711.2002.05415.x , https://ui.adsabs.harvard.edu/abs/2002MNRAS.333..411W 333, 411
Woudt P. A., Warner B., 2002, @doi [ ] 10.1046/j.1365-8711.2002.05415.x , https://ui.adsabs.harvard.edu/abs/2002MNRAS.333..411W 333, 411
2002
-
[62]
A., et al., 2012, @doi [ ] 10.1111/j.1365-2966.2012.22010.x , https://ui.adsabs.harvard.edu/abs/2012MNRAS.427.1004W 427, 1004
Woudt P. A., et al., 2012, @doi [ ] 10.1111/j.1365-2966.2012.22010.x , https://ui.adsabs.harvard.edu/abs/2012MNRAS.427.1004W 427, 1004
2012
-
[63]
R., G \"a nsicke B
Zorotovic M., Schreiber M. R., G \"a nsicke B. T., 2011, @doi [ ] 10.1051/0004-6361/201116626 , https://ui.adsabs.harvard.edu/abs/2011A&A...536A..42Z 536, A42
2011 doi
-
[64]
G., 2001, @doi [ ] 10.1086/323894 , https://ui.adsabs.harvard.edu/abs/2001PASP..113.1420V 113, 1420
van Dokkum P. G., 2001, @doi [ ] 10.1086/323894 , https://ui.adsabs.harvard.edu/abs/2001PASP..113.1420V 113, 1420
2001 doi
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