2007MNRAS.374..999J


Query : 2007MNRAS.374..999J

2007MNRAS.374..999J - Mon. Not. R. Astron. Soc., 374, 999-1005 (2007/January-3)

Detection of the radial velocity curve of the B5-A0 supergiant companion star of Cir X-1?

JONKER P.G., NELEMANS G. and BASSA C.G.

Abstract (from CDS):

In this paper, we report on phase-resolved I-band optical spectroscopic and photometric observations of Cir X-1 obtained with the Very Large Telescope. The spectra are dominated by Paschen absorption lines at nearly all orbital phases except near phase zero (coinciding with the X-ray dip) when the absorption lines are filled in by broad Paschen emission lines. The radial velocity curve of the absorption lines corresponds to an eccentric orbit (e = 0.45) whose period and time of periastron passage are consistent with the period and phase predicted by the most recent X-ray dip ephemeris. We found that the I-band magnitude decreases from 17.6 to ∼16.8 near phase 0.9-1.0; this brightening coincides in phase with the X-ray dip. Even though it is likely that the absorption-line spectrum is associated with the companion star of Cir X-1, we cannot exclude the possibility that the spectrum originates in the accretion disc. However, if the spectrum belongs to the companion star, it must be a supergiant of spectral type B5-A0. If we assume that the compact object does not move through the companion star at periastron, the companion star mass is constrained to ≲10 M☉for a 1.4-M☉ neutron star, whereas the inclination has to be. Alternatively, the measured absorption lines and their radial velocity curve can be associated with the accretion disc surrounding a 1.4-M☉neutron star and its motion around the centre of mass. An absorption-line spectrum from an accretion disc is typically found when our line of sight passes through the accretion disc rim implying a high inclination. In this scenario, the companion star mass is found to be ∼0.4 M☉. However, from radio observations it was found that the angle between the line of sight and the jet axis is smaller than 5°. This would mean that the jet ploughs through the accretion disc in this scenario, making this solution less probable.

Abstract Copyright: 2006 The Authors. Journal compilation © 2006 RAS

Journal keyword(s): accretion, accretion discs - stars: individual: Cir X-1 - stars: neutron - X-rays: binaries

Simbad objects: 16

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Number of rows : 16
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 HD 268623 s*b 04 52 19.0947780648 -66 43 53.320001052 10.709 11.51 11.61   11.482 B2Ia 48 0
2 HD 268749 s*b 04 53 29.3921844216 -69 24 32.868371052   12.14 12.10     B7Iab 17 0
3 HD 32034 s*b 04 55 11.0851969440 -67 10 10.411470552 9.13 9.756 9.715 9.70 9.51 B9Iae 81 0
4 HD 33579 sg* 05 05 55.5114721104 -67 53 10.932988848   9.32 9.13     A2Ia+ 148 0
5 HD 271163 * 05 18 51.7465663008 -65 41 22.427266812 11.187 11.6 9.984     B3Ia 38 0
6 HD 269697 s*y 05 31 38.4223359696 -67 28 11.562011760 10.99 10.69 10.28     F6Ia 64 0
7 * nu. Cnc SB* 09 02 44.2677118128 +24 27 10.392222600   5.404 5.447     A0III 205 0
8 V* V395 Car LXB 09 22 34.6761959832 -63 17 41.355773520 15.40 16.104 15.455     K0III 143 0
9 PG 0942-029 HS* 09 45 11.8538082624 -03 09 21.034933164 12.537 13.714 14.012 14.144 14.308 sdB 57 0
10 * eta Leo sg* 10 07 19.9523915176 +16 45 45.587968398 3.17 3.39 3.41 3.32 3.35 A0Ib 351 0
11 * rho Leo s*b 10 32 48.6703908997 +09 18 23.705339948 2.780 3.720 3.870 3.90 4.06 B1Iab 550 0
12 V* BR Cir HXB 15 20 40.8532547060 -57 10 00.206639033   21.4 21.4     B5-A0I 849 1
13 AX J1739.1-3020 HXB 17 39 11.5515537336 -30 20 37.787917704     14.40 13.91   O8.5Iab(f) 166 1
14 * 67 Oph s*b 18 00 38.7157893000 +02 55 53.633402904 3.34 3.96 3.93 3.84 3.81 B4Ib-II 422 0
15 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A7Ib 2253 4
16 V* V1341 Cyg LXB 21 44 41.1544345272 +38 19 17.066570988 15.00 15.13 14.68 15.00   A9III 1229 1

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