2002ApJ...565.1107P


Query : 2002ApJ...565.1107P

2002ApJ...565.1107P - Astrophys. J., 565, 1107-1133 (2002/February-1)

Evolutionary sequences for low- and intermediate-mass X-ray binaries.

PODSIADLOWSKI P., RAPPAPORT S. and PFAHL E.D.

Abstract (from CDS):

We present the results of a systematic study of the evolution of low- and intermediate-mass X-ray binaries (LMXBs and IMXBs). Using a standard Henyey-type stellar evolution code and a standard model for binary interactions, we have calculated 100 binary evolution sequences containing a neutron star and a normal-type companion star, where the initial mass of the secondary ranges from 0.6 to 7 M☉ and the initial orbital period from ∼4 hr to ∼100 days. This range samples the entire range of parameters one is likely to encounter for LMXBs and IMXBs. The sequences show an enormous variety of evolutionary histories and outcomes, where different mass transfer mechanisms dominate in different phases. Very few sequences resemble the classical evolution of cataclysmic variables, where the evolution is driven by magnetic braking and gravitational radiation alone. Many systems experience a phase of mass transfer on a thermal timescale and may briefly become detached immediately after this phase (for the more massive secondaries). In agreement with previous results (Tauris & Savonije (ref???)1999), we find that all sequences with (sub)giant donors up to ∼2 M☉ are stable against dynamical mass transfer. Sequences where the secondary has a radiative envelope are stable against dynamical mass transfer for initial masses up to ∼4 M☉. For higher initial masses, they experience a delayed dynamical instability after a stable phase of mass transfer lasting up to ∼106 yr. Systems where the initial orbital period is just below the bifurcation period of ∼18 hr evolve toward extremely short orbital periods (as short as ∼10 minutes). For a 1 M☉ secondary, the initial period range that leads to the formation of ultracompact systems (with minimum periods less than ∼40 minutes) is 13-18 hr. Since systems that start mass transfer in this period range are naturally produced as a result of tidal capture, this may explain the large fraction of ultracompact LMXBs observed in globular clusters. The implications of this study for our understanding of the population of X-ray binaries and the formation of millisecond pulsars are also discussed.

Abstract Copyright: ∼

Journal keyword(s): Stars: Binaries: Close - Stars: Pulsars: General - Stars: Neutron - Stars: White Dwarfs - X-Rays: Stars

CDS comments: Fig.18 : 1735-555 and 1658-29 not identified

Simbad objects: 33

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Number of rows : 33
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 NGC 104 GlC 00 24 05.359 -72 04 53.20     4.09     ~ 4158 0
2 V* UY Vol LXB 07 48 33.71 -67 45 07.7 16.10 17.00 16.9 16.7 17.05 ~ 660 0
3 V* V395 Car LXB 09 22 34.6761959832 -63 17 41.355773520 15.40 16.104 15.455     K0III 143 0
4 V* GR Mus LXB 12 57 37.1833002949 -69 17 18.996899563   19.40 19.1     ~ 275 0
5 M 5 GlC 15 18 33.22 +02 04 51.7     5.95     ~ 2095 0
6 V* V818 Sco LXB 16 19 55.0692669024 -15 38 25.017666540 11.60 12.40 11.1     Oev 1730 0
7 V* KZ TrA LXB 16 32 16.79 -67 27 39.3 17.40 18.60 18.5     ~ 626 1
8 V* V801 Ara LXB 16 40 55.5976953528 -53 45 04.948107156 17.50 18.20 17.5   17.07 ~ 921 0
9 M 13 GlC 16 41 41.634 +36 27 40.75     5.8     ~ 2291 0
10 V* HZ Her LXB 16 57 49.8110126616 +35 20 32.486555472 11.90 14.89 13.63 13.88   B3/6ep 2172 0
11 V* V2216 Oph LXB 17 31 44.17 -16 57 40.9 16.40 17.10 16.8     ~ 329 1
12 V* V2116 Oph Sy* 17 32 02.1532435416 -24 44 44.129169096   20.78 18.4     M6IIIe 719 1
13 V* V926 Sco LXB 17 38 58.2384053021 -44 27 00.699118812 16.90 17.70 17.5     ~ 480 0
14 3FHL J1746.2-2852 LXB 17 44 33.09 -28 44 27.0           ~ 559 0
15 Cl Terzan 5 Cl* 17 48 05.00 -24 46 48.0           ~ 948 1
16 4U 1746-371 LXB 17 50 12.66 -37 03 08.2     8.43     ~ 206 1
17 NGC 6441 GlC 17 50 13.06 -37 03 05.2           ~ 940 0
18 Granat 1747-312 LXB 17 50 46.862 -31 16 28.86           ~ 135 0
19 Cl Terzan 6 GlC 17 50 47.02873 -31 16 29.6900           ~ 214 0
20 NGC 6624 GlC 18 23 40.51 -30 21 39.7           ~ 939 1
21 X Sgr X-4 LXB 18 23 40.57 -30 21 40.6   19.06 18.81     ~ 1056 1
22 V* V691 CrA LXB 18 25 46.8185061768 -37 06 18.529336656 14.30 15.20 15.1     ~ 461 0
23 Cl* NGC 6652 SAW V10 LXB 18 35 43.9 -32 59 18     18.9     ~ 104 0
24 NGC 6652 GlC 18 35 45.63 -32 59 26.6           ~ 474 0
25 NGC 6712 GlC 18 53 04.32 -08 42 21.5           ~ 550 0
26 4U 1850-086 LXB 18 53 04.89 -08 42 19.7 20.40 21.20 21.0     ~ 266 1
27 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A7Ib 2253 4
28 V* V1405 Aql LXB 19 18 47.6 -05 14 18 20.90 21.40 21.0     ~ 495 0
29 PSR J1959+2048 Psr 19 59 36.7643141520 +20 48 14.896407996   21.08 20.16 19.53 18.79 G: 854 3
30 4U 2129+12 LXB 21 29 58.3124 +12 10 02.670 14.50 15.70 15.8     ~ 326 1
31 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0
32 V* V1727 Cyg LXB 21 31 26.2133156448 +47 17 24.512055396 16.75 17.05 16.4     ~ 250 0
33 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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