2025A&A...702A.225C


Query : 2025A&A...702A.225C

2025A&A...702A.225C - Astronomy and Astrophysics, volume 702A225 (2025/10-1)

Characterising the short-orbital period X-ray transient Swift J1910.2-0546.

CORRAL-SANTANA J.M., RODRIGUEZ-GIL P., TORRES M.A.P., CASARES J., JONKER P.G., PERDOMO GARCIA A., TRELAWNY D.T., CARBALLO-BELLO J.A., CHARLES P.A., MATA SANCHEZ D., MUNOZ-DARIAS T., RINGWALD F.A., MARTINEZ-PAIS I.G., CORRADI R.L.M., SAIKIA P. and RUSSELL D.M.

Abstract (from CDS):

Context.Swift J1910.2-0546 (=MAXI J1910-057) is a Galactic X-ray transient discovered during a bright outburst in 2012. Its X-ray spectral and timing properties point to a black-hole accretor, yet the orbital period remains uncertain, and no reliable dynamical constraints on the binary parameters are available. The 2012 event, extensively monitored at X-ray and optical wavelengths, offers a rare opportunity to investigate the structure and dynamics of the system and to constrain its fundamental properties.
Aims. We use time-series optical photometry and spectroscopy, obtained during outburst and quiescence, to estimate the orbital period, characterise the donor star, determine the interstellar extinction, distance, and system geometry, and constrain the component masses.
Methods. Multi-site r-band and clear-filter light curves and WHT/ACAM spectra from the 2012 outburst were combined with time-series spectroscopy from GTC/OSIRIS and VLT/FORS2 in quiescence. Period searches were conducted using generalised Lomb-Scargle, phase-dispersion minimisation, and analysis-of-variance algorithms. We used diffuse interstellar bands to constrain E(B - V), while empirical correlations involving Hα yielded estimates of K2, q, and i.
Results. We detected a coherent, double-humped modulation with a period of 0.0941 ± 0.0007 d (2.26 ± 0.02 h) during the outburst. Its morphology is consistent with an early superhump, suggesting that the true orbital period may be slightly shorter than 4.52 h. The Hα radial velocity curves do not yield a definitive orbital period. In quiescence, TiO bands indicate an M3-M3.5 donor contributing ≃70% of the red continuum. Diffuse interstellar bands give E(B - V) = 0.60 ± 0.05 and NH = (3.9 ± 1.3)×1021 cm–2, placing the system at a distance of 2.8-4.0 kpc. The Hα line width in quiescence (FWHM0 = 990 ± 45 km s–1), via a FWHM-K2 calibration, provides an estimate of K2, while its double-peaked profile gives q and the orbital inclination. The latter appears much higher than estimates from X-ray studies. Adopting the resulting K2 = 230 ± 17 km s–1 and q = 0.032 ± 0.010, along with two orbital period scenarios (2.25 and 4.50 h), Monte Carlo sampling returns a compact object mass of M1 = 8 - 11 M⊙ and an inclination of i = 13° -18° for plausible donor masses (M2 = 0.25 - 0.35 M⊙). Overall, we favour an orbital period of 4.5 h.
Conclusions.Swift J1910.2-0546 may be a short-period, low-inclination black hole X-ray transient, although the possibility of it being a neutron star accretor cannot be completely ruled out. Subsequent phase-resolved spectroscopy and photometry during quiescence are needed to better determine its fundamental parameters.

Abstract Copyright: © The Authors 2025

Journal keyword(s): accretion, accretion disks - binaries: close - stars: black holes - stars: individual: Swift J1910.2-0546 - X-rays: binaries

Simbad objects: 25

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Number of rows : 25
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* VX Ari PM* 02 44 15.5097410539 +25 31 24.114854200 13.363 12.141 10.563 9.49 8.115 dM3 249 0
2 BD+05 1668 PM* 07 27 24.4989685603 +05 13 32.841491057 12.558 11.443 9.872 8.699 7.161 M3.5V 477 0
3 V* YZ CMi PM* 07 44 40.1723046464 +03 33 08.875227574 13.761 12.831 11.225 9.958 8.263 M4.0Ve 957 0
4 Ross 619 PM* 08 11 57.5691729379 +08 46 22.952885566   14.60 12.834 12.527   M4.5V 227 0
5 BD+02 2098 PM* 08 55 07.6217256509 +01 32 47.415143239 12.642 11.30 9.997 9.072 8.204 M0V 125 1
6 MCC 568 ** 10 12 04.6719766322 -02 41 05.170732851 13.415 12.205 10.629 9.581 8.303 M2.5V 116 0
7 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
8 BD+25 2534 HS* 12 37 23.5161671712 +25 03 59.867922240 9.117 10.26 10.59 10.642 10.809 sdB1(k) 268 0
9 HD 111631 PM* 12 50 43.5668194245 -00 46 05.267733737 11.187 9.892 8.470 7.59 6.752 M0V 247 0
10 HD 119850 PM* 13 45 43.7755597223 +14 53 29.471707437 10.989 9.894 8.50 7.465 6.363 M2V 402 0
11 HD 125455B PM* 14 19 35.8445765349 -05 09 08.321917565   16.0 14.5     M4.0V 49 1
12 LP 802-68 PM* 15 24 45.7511566260 -17 07 39.343095435   12.37 13.738 11.410   M2V 35 0
13 MAXI J1659-152 LXB 16 59 01.680 -15 15 28.73           ~ 274 0
14 V* V1239 Her CV* 17 02 13.2462561912 +32 29 54.159948960           M1.5e 60 0
15 G 19-15 ** 17 11 52.25370 -01 51 06.3227 14.28 13.005 11.393 10.286 8.877 M3V 80 0
16 MAXI J1820+070 LXB 18 20 21.9423816480 +07 11 07.284859440           ~ 511 0
17 MAXI J1836-194 XB* 18 35 43.440 -19 19 10.48           ~ 163 0
18 CD-44 12736 PM* 18 36 25.9502475648 -44 18 36.907592904   10.83 10.22     G0 222 0
19 Gaia DR3 4206052097085749760 * 19 10 20.1640193998 -05 48 09.343410736           ~ 1 0
20 MAXI J1910-057 LXB 19 10 22.80 -05 47 55.9           ~ 84 0
21 CD-27 14169 PM* 19 39 36.1703597866 -26 45 07.072666448 13.104 11.895 10.482 9.561 8.576 M1V 32 0
22 V* WZ Sge CV* 20 07 36.5037622512 +17 42 14.733254952   15.30 15.20 10.817   D 982 0
23 V* V503 Cyg CV* 20 27 17.3992939944 +43 41 22.504607556           ~ 138 0
24 HD 209290 PM* 22 02 10.2750978279 +01 24 00.832158070 11.838 10.616 9.146 8.213 7.245 M0.5V 285 0
25 V* EZ Aqr Er* 22 38 33.576000 -15 17 59.75700 15.762 14.33 12.38 12.12 8.677 M5V 320 1

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