2014A&A...561A..11V


Query : 2014A&A...561A..11V

2014A&A...561A..11V - Astronomy and Astrophysics, volume 561A, 11-11 (2014/1-1)

On the disruption of pulsar and X-ray binaries in globular clusters.

VERBUNT F. and FREIRE P.C.C.

Abstract (from CDS):

The stellar encounter rate Γ has been shown to be strongly correlated with the number of X-ray binaries in globular clusters (GCs) and also to the number of radio pulsars. However, the pulsar populations in different GCs show remarkably different characteristics: in some GCs the population is dominated by binary systems, in others by single pulsars and exotic systems that result from exchange encounters. In this paper, we describe a second dynamical parameter for GCs, the encounter rate for a single binary, γ. We find that this parameter provides a good characterization of the differences between the pulsar populations of different GCs. The higher γ is for any particular GC, the more isolated pulsars and products of exchange interactions are observed. Furthermore, we also find that slow and ``young'' pulsars are found almost exclusively in clusters with a high γ; this suggests that these kinds of objects are formed by the disruption of X-ray binaries, thus halting the recycling of a previously dead neutron star. We discuss the implications of this for the nature of young pulsars and for the formation of neutron stars in GCs.

Abstract Copyright:

Journal keyword(s): globular clusters: general - stars: neutron - pulsars: general

Simbad objects: 35

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Number of rows : 35
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 NGC 104 GlC 00 24 05.359 -72 04 53.20     4.09     ~ 3914 0
2 PSR J0407+16 Psr 04 07 54.939 +16 07 16.40           ~ 31 1
3 PSR J0514-4002A Psr 05 14 06.6927 -40 02 48.897           ~ 52 1
4 NGC 1851 GlC 05 14 06.76 -40 02 47.6           ~ 1429 0
5 M 53 GlC 13 12 55.25 +18 10 05.4     7.79     ~ 836 0
6 M 3 GlC 13 42 11.62 +28 22 38.2     6.39     ~ 2478 0
7 M 5 GlC 15 18 33.22 +02 04 51.7     5.95     ~ 1977 0
8 M 4 GlC 16 23 35.22 -26 31 32.7           ~ 1848 0
9 M 13 GlC 16 41 41.634 +36 27 40.75     5.8     ~ 2191 0
10 M 62 GlC 17 01 12.60 -30 06 44.5           ~ 619 0
11 PSR B1718-19 Psr 17 21 01.48 -19 36 51.0           ~ 91 1
12 NGC 6342 GlC 17 21 10.14 -19 35 14.7     10.01     ~ 286 0
13 NGC 6397 GlC 17 40 42.09 -53 40 27.6     5.17     ~ 1975 0
14 PSR J1740-5340 Psr 17 40 44.589 -53 40 40.90   17.43   16.25   ~ 148 2
15 PSR J1748-2446ad Psr 17 48 04.9 -24 46 04           ~ 121 1
16 Cl Terzan 5 Cl* 17 48 05.00 -24 46 48.0           ~ 845 1
17 NGC 6440 GlC 17 48 52.67 -20 21 34.5           ~ 550 0
18 PSR B1745-20A Psr 17 48 52.689 -20 21 39.70     10.55     ~ 46 1
19 NGC 6441 GlC 17 50 13.06 -37 03 05.2           ~ 884 0
20 NGC 6517 GlC 18 01 50.376 -08 57 34.39   11.08       ~ 182 0
21 NGC 6522 GlC 18 03 34.08 -30 02 02.3           ~ 524 0
22 NGC 6544 GlC 18 07 20.58 -24 59 50.4   11.36 9.90     ~ 296 0
23 PSR J1807-2500B Psr 18 07 20.871209 -25 00 01.91500           ~ 51 0
24 NGC 6624 GlC 18 23 40.51 -30 21 39.7           ~ 885 1
25 PSR J1823-3021C Psr 18 23 41.1516 -30 21 38.450           ~ 13 0
26 PSR B1820-30B Psr 18 23 41.538 -30 21 41.70           ~ 50 0
27 PSR J1824-2452A Psr 18 24 32.009 -24 52 11.10           ~ 499 2
28 M 28 GlC 18 24 32.89 -24 52 11.4           ~ 768 0
29 NGC 6749 OpC 19 05 15.36 +01 54 00.0     12.4     ~ 157 0
30 NGC 6752 GlC 19 10 52.11 -59 59 04.4           ~ 2000 0
31 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 989 1
32 M 71 GlC 19 53 46.49 +18 46 45.1           ~ 1127 0
33 PSR J2016+1948 Psr 20 16 56.7 +19 48 03           ~ 18 1
34 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3138 0
35 PSR J2129+1209C Psr 21 30 01.2030 +12 10 38.159           ~ 194 2

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