The impact of stellar evolution on rotating star clusters: the gravothermal-gravogyro catastrophe and the formation of a bar of black holes

  • A W H Kamlah
    Max-Planck-Institut für Astronomie , Königstuhl 17, D-69117 Heidelberg, Germany
  • R Spurzem
    Astronomisches Rechen-Institut, Zentrum für Astronomie, University of Heidelberg , Mönchhofstrasse 12-14, D-69120 Heidelberg, Germany
  • P Berczik
    Astronomisches Rechen-Institut, Zentrum für Astronomie, University of Heidelberg , Mönchhofstrasse 12-14, D-69120 Heidelberg, Germany
  • M Arca Sedda
    Astronomisches Rechen-Institut, Zentrum für Astronomie, University of Heidelberg , Mönchhofstrasse 12-14, D-69120 Heidelberg, Germany
  • F Flammini Dotti
    Astronomisches Rechen-Institut, Zentrum für Astronomie, University of Heidelberg , Mönchhofstrasse 12-14, D-69120 Heidelberg, Germany
  • N Neumayer
    Max-Planck-Institut für Astronomie , Königstuhl 17, D-69117 Heidelberg, Germany
  • X Pang
    Department of Physics, Xi’an Jiaotong-Liverpool University , 111 Ren’ai Rd., Suzhou Dushu Lake Science and Education Innovation District, Suzhou Industrial Park, Suzhou 215123, China
  • Q Shu
    Kavli Institute for Astronomy and Astrophysics, Peking University , Yiheyuan Lu 5, Haidian Qu, Beijing 100871, China
  • A Tanikawa
    Department of Earth Science and Astronomy, College of Arts and Sciences, The University of Tokyo , 3-8-1 Komaba, Meguro-ku, Tokyo 153-8902, Japan
  • M Giersz
    Nicolaus Copernicus Astronomical Centre, Polish Academy of Sciences , ul. Bartycka 18, PL-00-716 Warsaw, Poland

説明

<jats:title>ABSTRACT</jats:title> <jats:p>We present results from a suite of eight direct N-body simulations, performed with nbody6++ GPU, representing realistic models of rotating star clusters with up to 1.1 × 105 stars. Our models feature primordial (hard) binaries, a continuous mass spectrum, differential rotation, and tidal mass-loss induced by the overall gravitational field of the host galaxy. We explore the impact of rotation and stellar evolution on the star cluster dynamics. In all runs for rotating star clusters, we detect a previously predicted mechanism: an initial phase of violent relaxation followed by the so-called gravogyro catastrophe. We find that the gravogyro catastrophe reaches a finite amplitude, which depends in strength on the level of the bulk rotation, and then levels off. After this phase, the angular momentum is transferred from high-mass to low-mass particles in the cluster (both stars and compact objects). Simultaneously, the system becomes gravothermally unstable and collapses, thus undergoing the so-called gravothermal-gravogyro catastrophe. Comparing models with and without stellar evolution, we find an interesting difference. When stellar evolution is not considered, the whole process proceeds at a faster pace. The population of heavy objects tends to form a triaxial structure that rotates in the cluster centre. When stellar evolution is considered, we find that such a rotating bar is populated by stellar black holes and their progenitors. The triaxial structure becomes axisymmetric over time, but we also find that the models without stellar evolution suffer repeated gravogyro catastrophes as sufficient angular momentum and mass are removed by the tidal field.</jats:p>

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