2002A&A...392..909C


Query : 2002A&A...392..909C

2002A&A...392..909C - Astronomy and Astrophysics, volume 392, 909-920 (2002/9-4)

Physical parameters of the high-mass X-ray binary 4U 1700-37.

CLARK J.S., GOODWIN S.P., CROWTHER P.A., KAPER L., FAIRBAIRN M., LANGER N. and BROCKSOPP C.

Abstract (from CDS):

We present the results of a detailed non-LTE analysis of the ultraviolet and optical spectrum of the O6.5Iaf+ star HD 153919 - the mass donor in the high-mass X-ray binary 4U 1700-37. We find that the star has a luminosity log(L*/L)=5.82±0.07, Teff=35000±1000K, radius R*=21.9+1.3–0.5R, mass-loss rate {dot}(M)=9.5x10–6M/yr, and a significant overabundance of nitrogen (and possibly carbon) relative to solar values. Given the eclipsing nature of the system these results allow us to determine the most likely masses of both components of the binary via Monte Carlo simulations. These suggest a mass for HD 153919 of M*=58±11M - implying the initial mass of the companion was rather high (>60M). The most likely mass for the compact companion is found to be Mx=2.44±0.27M, with only 3.5 per cent of the trials resulting in a mass less than 2.0M and none less than 1.65M. Such a value is significantly in excess of the upper observational limit to the masses of neutron stars of 1.45M found by Thorsett & Chakrabarthy (1999ApJ...512..288T), although a mass of 1.86M has recently been reported for the Vela X-1 pulsar (Barziv et al., 2001A&A...377..925B). Our observational data is inconsistent with the canonical neutron star mass and the lowest black hole mass observed (>4.4M; Nova Vel). Significantly changing observational parameters can force the compact object mass into either of these regimes but, given the strong proportionality between M* and Mx, the O-star mass changes by factors of greater than 2, well beyond the limits determined from its evolutionary state and surface gravity. The low mass of the compact object implies that it is difficult to form high mass black holes through both the Case A & B mass transfer channels and, if the compact object is a neutron star, would significantly constrain the high density nuclear equation of state.

Abstract Copyright:

Journal keyword(s): stars: early-type - stars: individual: HD 153919, 4U 1700-37 - X-rays: stars - stars: binaries: general

CDS comments: In fig. 7 J0422+32 = GRO J0422+32.

Simbad objects: 38

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Number of rows : 38
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 PSR J0045-7319 Psr 00 45 35.2606875816 -73 19 03.269105220   15.97 16.18   16.30 B0.5-B2IV-V 183 0
2 SK 160 HXB 01 17 05.1457288392 -73 26 36.014808156 12.23 13.00 13.15   13.17 O9.7Ia+ 858 0
3 V* V518 Per HXB 04 21 42.7227473352 +32 54 26.939156184 13.00 13.50 13.2     M4.5V 651 1
4 X LMC X-4 HXB 05 32 49.5556042296 -66 22 13.202721768   13.9 14.0     O8III 668 0
5 X LMC X-3 HXB 05 38 56.6323605504 -64 05 03.317937504   17 17.2     B2.5Ve 675 0
6 1A 0620-00 HXB 06 22 44.5423857312 -00 20 44.290460544 10.60 11.40 11.2     K3V-K7V 1113 0
7 HD 63099 WR* 07 45 50.3991805440 -34 19 48.500286780 11.47 11.43 10.50 10.37   WC4+O7 112 0
8 NAME Vela XYZ Rad 08 34.0 -45 50           ~ 1229 2
9 V* GP Vel HXB 09 02 06.8608812864 -40 33 16.899168060 6.85 7.37 6.87 6.31 6.05 B0.5Ia 1503 0
10 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 379 1
11 V* MM Vel HXB 10 13 36.4108035720 -45 04 32.553865524   14.84 14.71     G5V-M0V 198 0
12 HD 97152 WR* 11 10 04.0797150120 -60 58 44.963276664 7.47 8.03 8.07 8.91   WC7+O7V 183 0
13 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120     12.25     K5V-M1V 822 0
14 V* V779 Cen HXB 11 21 15.0920532528 -60 37 25.630264596   14.4 12.27     O9III/Veq 1096 0
15 V* GU Mus HXB 11 26 26.5961559600 -68 40 32.877752952           K3V-K7V 715 1
16 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 429 1
17 V* QV Nor HXB 15 42 23.3633146128 -52 23 09.577395960   16.3 14.5     B0.2Ia:e 420 1
18 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760     11.96     ~ 493 1
19 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000   17.95 16.6     K3III 1172 0
20 NAME Sco OB 1 As* 16 53.5 -41 57           ~ 217 0
21 V* V1033 Sco HXB 16 54 00.137 -39 50 44.90   15.20 14.2 16.14   F5IV 1886 1
22 HD 152270 WR* 16 54 19.6991292072 -41 49 11.531710092 6.26 6.80 6.597 6.72 6.39 WC7+O5-8 303 0
23 V* HZ Her LXB 16 57 49.8110126616 +35 20 32.486555472 11.90 14.89 13.63 13.88   B3/6ep 2076 0
24 HD 153919 HXB 17 03 56.7725629224 -37 50 38.913331452 6.06 6.78 6.51 6.08 5.90 O6Iafcp 813 1
25 V* V2107 Oph HXB 17 08 14.520 -25 05 30.15   16.50 15.9     K3V-K7V 226 1
26 PSR J1713+0747 Psr 17 13 49.5331917 +07 47 37.492580           ~ 464 1
27 PSR J1802-07 Psr 18 04 49.8954 -07 35 24.690     12.33     ~ 97 2
28 V* V4641 Sgr HXB 18 19 21.6343259256 -25 24 25.849595952     13.654   13.092 B9III 472 1
29 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 530 1
30 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2627 0
31 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 989 1
32 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4334 0
33 V* QZ Vul HXB 20 02 49.58 +25 14 11.3   19.64 18.2     K3V-K6V 421 0
34 V* V404 Cyg HXB 20 24 03.8254458776 +33 52 01.962185735           G9/K0III/V 1275 0
35 PSR B2127+11 Psr 21 29 58.24650 +12 10 01.2339           ~ 97 2
36 V* V1341 Cyg LXB 21 44 41.1544345272 +38 19 17.066570988 15.00 15.13 14.68 15.00   A9III 1155 1
37 HD 214419 WR* 22 36 53.9548302648 +56 54 20.989190232 8.68 9.376 8.996 8.962   WN6o+O9Ib/II 377 1
38 PSR J2305+4707 Psr 23 05 55.842 +47 07 45.32           ~ 220 1

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