2000A&A...364..563V


Query : 2000A&A...364..563V

2000A&A...364..563V - Astronomy and Astrophysics, volume 364563-572 (2000/12-2)

On the origin of the difference between the runaway velocities of the OB-supergiant X-ray binaries and the Be/X-ray binaries.

VAN DEN HEUVEL E.P.J., PORTEGIES ZWART S.F., BHATTACHARYA D. and KAPER L.

Abstract (from CDS):

The recent finding by Chevalier & Ilovaisky (1998A&A...330..201C) from Hipparcos observations that OB-supergiant X-ray binaries have relatively large runaway velocities (mean peculiar tangential velocity <vtr≥42±14km/s), whereas Be/X-ray binaries have low runaway velocities (<vtr≥15±6km/s), provides confirmation of the current models for the formation of these two types of systems. These predict a difference in runaway velocity of this order of magnitude. This difference basically results from the variation of the fractional helium core mass as a function of stellar mass, in combination with the conservation of orbital angular momentum during the mass transfer phase that preceded the formation of the compact object in the system. This combination results into: (i) Systematically narrower pre-supernova orbits in the OB-supergiant systems than in the Be-systems, and (ii) A larger fractional amount of mass ejected in the supernovae in high-mass systems relative to systems of lower mass. Regardless of possible kick velocities imparted to neutron stars at birth, this combination leads to a considerable difference in average runaway velocity between these two groups. If one includes the possibility for non-conservative mass transfer the predicted difference between the runaway velocity of the two groups becomes even more pronounced. The observed low runaway velocities of the Be/X-ray binaries confirm that in most cases not more than 1 to 2M☉ was ejected in the supernovae that produced their neutron stars. This, in combination with the -on average- large orbital eccentricities of these systems, indicates that their neutron stars must have received a velocity kick in the range 60-250km/s at birth. The considerable runaway velocity of Cygnus X-1 (vtr=50±15km/s) shows that also with the formation of a black hole considerable mass ejection takes place.

Abstract Copyright: ∼

Journal keyword(s): stars: binaries: close - stars: early-type - stars: emission-line, Be - stars: evolution - stars: supernovae: general - X-rays: stars

CDS comments: Table 3: PSR J1259-63 misprint for PSR B1259-63 = PSR J1302-6350

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 PSR J0045-7319 HXB 00 45 35.2606875816 -73 19 03.269105220   15.97 16.18   16.30 B0.5-B2IV-V 193 0
2 V* V662 Cas HXB 01 18 02.6976641952 +65 17 29.829200388 12.27 11.99 11.14 10.33 9.58 B1Iae 289 0
3 V* V635 Cas HXB 01 18 31.9704955824 +63 44 33.072603144 17.05 16.64 15.19 14.34 13.22 B0.2Ve 791 0
4 LS I +61 303 HXB 02 40 31.6644419688 +61 13 45.593918580 11.27 11.61 10.75 10.19 9.55 B0Ve 903 2
5 V* BQ Cam HXB 03 34 59.9116110096 +53 10 23.296879776   17.16 15.42 14.26 13.04 O8.5Ve 525 1
6 V* X Per HXB 03 55 23.0777456088 +31 02 45.039836148 6.090 6.840 6.720     O9.5III 1037 0
7 HD 34921 HXB 05 22 35.2313961840 +37 40 33.638562768 6.78 7.64 7.48     B0IVpe 140 0
8 HD 269806 * 05 34 55.8715804968 -66 53 55.921014096 10.94 10.95 10.40     G0 11 0
9 HD 37241 ** 05 38 17.1210572472 +26 55 01.233734988   9.28 8.80     G0 10 0
10 HD 245770 HXB 05 38 54.5748918624 +26 18 56.836952784 9.30 9.84 9.39 8.77 8.30 O9/B0III/Ve 1045 0
11 HD 63666 HXB 07 47 23.5848942480 -53 19 56.822589048   7.60 7.60     B7IV/V 40 0
12 HD 65663 Be* 07 56 15.7697008 -61 05 57.949993 6.54 6.723 6.730     B8V 55 1
13 V* GP Vel HXB 09 02 06.8608812864 -40 33 16.899168060 6.85 7.37 6.87 6.31 6.05 B0.5Ia 1588 0
14 HD 91188 Be* 10 30 22.4122667064 -57 04 38.604393876 5.98 6.491 6.615     B5IIIe 55 0
15 LS 1698 HXB 10 37 35.3145142200 -56 47 55.869594756   12.00 11.48 11.38   B0III-Ve 120 0
16 HD 102567 HXB 11 48 00.0214464120 -62 12 24.902384760 8.24 9.06 9.00 9.62   B1Vne 335 0
17 HD 109857 Be* 12 39 14.57557 -75 22 14.1384 6.33         B8Vn 73 0
18 HD 110432 HXB 12 42 50.2663572384 -63 03 31.052981412 4.79 5.58 5.31     B0.5IVpe 334 0
19 * mu.02 Cru Be* 12 54 36.8841589536 -57 10 07.193918388 4.59 5.09 5.20 5.00 5.06 B5Vne 189 0
20 V* V850 Cen HXB 13 01 17.0968941216 -61 36 06.637549788   15.6 14.40     B2Vne 361 0
21 CPD-63 2495 HXB 13 02 47.6544015048 -63 50 08.626970292 10.34 10.72 9.98 10.03   O9.5Ve 852 0
22 V* QV Nor HXB 15 42 23.3633146128 -52 23 09.577395960   16.3 14.5     B0.2Ia 455 1
23 HD 153919 HXB 17 03 56.7725629224 -37 50 38.913331452 6.06 6.78 6.51 6.08 5.90 O6Iafcp 851 0
24 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
25 V* V2246 Cyg HXB 20 32 15.2749858128 +37 38 14.843024844   22.16 19.41 17.32 15.18 B0Ve 480 0

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