2011ApJ...732...67M


Query : 2011ApJ...732...67M

2011ApJ...732...67M - Astrophys. J., 732, 67 (2011/May-2)

Fokker-planck models for M15 without a central black hole: the role of the mass function.

MURPHY B.W., COHN H.N. and LUGGER P.M.

Abstract (from CDS):

We have developed a set of dynamically evolving Fokker-Planck models for the collapsed-core globular star cluster M15, which directly address the issue of whether a central black hole is required to fit Hubble Space Telescope (HST) observations of the stellar spatial distribution and kinematics. As in our previous work reported by Dull et al., we find that a central black hole is not needed. Using local mass-function data from HST studies, we have also inferred the global initial stellar mass function. As a consequence of extreme mass segregation, the local mass functions differ from the global mass function at every location. In addition to reproducing the observed mass functions, the models also provide good fits to the star-count and velocity-dispersion profiles, and to the millisecond pulsar accelerations. We address concerns about the large neutron star populations adopted in our previous Fokker-Planck models for M15. We find that good model fits can be obtained with as few as 1600 neutron stars; this corresponds to a retention fraction of 5% of the initial population for our best-fit initial mass function. The models contain a substantial population of massive white dwarfs, that range in mass up to 1.2M☉. The combined contribution by the massive white dwarfs and neutron stars provides the gravitational potential needed to reproduce HST measurements of the central velocity-dispersion profile.

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Journal keyword(s): globular clusters: general - globular clusters: individual: M15 - stars: kinematics and dynamics - stars: luminosity function, mass function

Simbad objects: 11

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Number of rows : 11
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 M 4 GlC 16 23 35.22 -26 31 32.7           ~ 1978 0
3 NGC 6397 GlC 17 40 42.09 -53 40 27.6     5.17     ~ 2103 0
4 M 71 GlC 19 53 46.49 +18 46 45.1           ~ 1190 0
5 CXOU J212958.1+121002 XB* 21 29 58.06 +12 10 02.6     16.6     ~ 87 1
6 [WA2001] M 15 X-3 X 21 29 58.155 +12 09 40.04           ~ 23 0
7 PSR B2127+11 Psr 21 29 58.24650 +12 10 01.2339           ~ 102 2
8 PSR J2129+1210D Psr 21 29 58.274 +12 09 59.74           ~ 31 0
9 4U 2129+12 LXB 21 29 58.3124 +12 10 02.670 14.50 15.70 15.8     ~ 326 1
10 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0
11 M 30 GlC 21 40 22.12 -23 10 47.5     7.10     ~ 1121 0

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