Dynamical stability of N-body models for M32 with a central black hole

被引:12
|
作者
vanderMarel, RP
Sigurdsson, S
Hernquist, L
机构
[1] UNIV CAMBRIDGE, INST ASTRON, CAMBRIDGE CB3 0HA, ENGLAND
[2] UNIV CALIF SANTA CRUZ, DEPT ASTRON & ASTROPHYS, SANTA CRUZ, CA 95064 USA
来源
ASTROPHYSICAL JOURNAL | 1997年 / 487卷 / 01期
关键词
black hole physics; galaxies; elliptical and lenticular; cD; individual; (M32); kinematics and dynamics; nuclei; structure;
D O I
10.1086/304605
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We study the stability of stellar dynamical equilibrium models for M32. Kinematic observations show that M32 has a central dark mass of similar to 3 x 10(6) M., most likely a black hole, and a phase-space distribution function that is close to the ''two-integral'' form f = f(E, L-z). M32 is also rapidly rotating; 85%-90% of the stars have the same sense of rotation around the symmetry axis. Previous work has shown that flattened, rapidly rotating two-integral models can be bar-unstable. We have performed N-body simulations to test whether this is the case for M32. This is the first stability analysis of two-integral models that have both a central density cusp and a nuclear black hole. Particle realizations with N = 512,000 were generated from distribution functions that fit the photometric and kinematic data of M32. We constructed equal-mass particle realizations and also realizations with a mass spectrum to improve the central resolution. Models were studied for two representative inclinations, i = 90 degrees (edge-on) and i = 55 degrees, corresponding to intrinsic axial ratios of q = 0.73 and q = 0.55, respectively. The time evolution of the models was calculated with a ''self-consistent field'' code on a Gray T3D parallel supercomputer. We find both models to be dynamically stable. This implies that they provide a physically meaningful description of M32 and that the inclination of M32 (and hence its intrinsic flattening) cannot be strongly constrained through stability arguments. Previous work on the stability of f(E, L-z) models has shown that the bar mode is the most common unstable mode for systems rounder than q approximate to 0.3 (i.e., E7) and that the likelihood for this mode to be unstable increases with flattening and rotation rate. The f(E, L-z) models studied for M32 are not bar-unstable, and M32 has a higher rotation rate than nearly all other elliptical galaxies. This suggests that f(E, L-z) models constructed to fit data for real elliptical galaxies will generally be stable, at least for systems rounder than q greater than or similar to 0.55, and possibly for flatter systems as well.
引用
收藏
页码:153 / 162
页数:10
相关论文
共 50 条
  • [1] A CENTRAL BLACK-HOLE IN M32
    TONRY, JL
    ASTROPHYSICAL JOURNAL, 1987, 322 (02): : 632 - 642
  • [2] A SAURON study of M32: measuring the intrinsic flattening and the central black hole mass
    Verolme, EK
    Cappellari, M
    Copin, Y
    van der Marel, RP
    Bacon, R
    Bureau, M
    Davies, RL
    Miller, BM
    de Zeeuw, PT
    MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 2002, 335 (03) : 517 - 525
  • [3] AXISYMMETRICAL GALAXY MODELS WITH CENTRAL BLACK-HOLES, WITH AN APPLICATION TO M32
    QIAN, EE
    DEZEEUW, PT
    VANDERMAREL, RP
    HUNTER, C
    MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 1995, 274 (02) : 602 - 622
  • [4] A massive black hole at the centre of the quiescent galaxy M32
    Roeland P. van der Marel
    P. Tim de Zeeuw
    Hans-Walter Rix
    Gerald D. Quinlan
    Nature, 1997, 385 : 610 - 612
  • [5] Improved evidence for a black hole in M32 from HST/FOS spectra. II. Axisymmetric dynamical models
    van der Marel, RP
    Cretton, N
    de Zeeuw, P
    Rix, HW
    ASTROPHYSICAL JOURNAL, 1998, 493 (02): : 613 - 631
  • [6] A massive black hole at the centre of the quiescent galaxy M32
    vanderMarel, RP
    deZeeuw, PT
    Rix, HW
    Quinlan, GD
    NATURE, 1997, 385 (6617) : 610 - 612
  • [7] DYNAMICAL MODELS OF M87 WITHOUT A CENTRAL BLACK-HOLE
    RICHSTONE, DO
    TREMAINE, S
    ASTROPHYSICAL JOURNAL, 1985, 296 (02): : 370 - 378
  • [8] A Dynamical N-body model for the central region of ω Centauri
    Jalali, B.
    Baumgardt, H.
    Kissler-Patig, M.
    Gebhardt, K.
    Noyola, E.
    Luetzgendorf, N.
    de Zeeuw, P. T.
    ASTRONOMY & ASTROPHYSICS, 2012, 538
  • [10] HST/FOS spectra of the nucleus of M32: Improved evidence for a nuclear black hole
    van der Marel, RP
    SECOND STROMLO SYMPOSIUM: THE NATURE OF ELLIPTICAL GALAXIES, 1997, 116 : 138 - 141