Resonant trapping of stars by merging massive black hole binaries

A massive black hole binary might resonantly trap a star (e.g. a white dwarf) and the gas released by its tidal disruption might emit electromagnetic wave signals around the coalescence of the binary. With post-Newtonian equations of motion including gravitational radiation reaction, we numerically studied resonant trappings by black hole binaries with a mass ratio of 1/100. It is found that 2:1 (and simultaneously 4:2) mean motion resonances of the binaries would be strong and could, in principle, draw small third objects deep into relativistic regimes (e.g. ∼10 Schwarzschild radii). The inclinations of the trapped objects could increase significantly and, in some cases, retrograde orbits could be realized eventually.

[1]  On disc driven inward migration of resonantly coupled planets with application to the system around GJ876 , 2001, astro-ph/0104432.

[2]  Jon M. Jenkins,et al.  ARCHITECTURE AND DYNAMICS OF KEPLER'S CANDIDATE MULTIPLE TRANSITING PLANET SYSTEMS , 2011, 1102.0543.

[3]  Martin J. Rees,et al.  Tidal disruption of stars by black holes of 106–108 solar masses in nearby galaxies , 1988, Nature.

[4]  Matthew Holman,et al.  Long-Term Stability of Planets in Binary Systems , 1996 .

[5]  G. Schäfer Three-body hamiltonian in general relativity , 1987 .

[6]  N. Gorelick,et al.  Mean Motion Resonances from Planet-Planet Scattering , 2008, 0809.3449.

[7]  C. Murray,et al.  Solar System Dynamics: Expansion of the Disturbing Function , 1999 .

[8]  A. Loeb,et al.  Prompt Tidal Disruption of Stars as an Electromagnetic Signature of Supermassive Black Hole Coalescence , 2010, 1004.4833.

[9]  William H. Press,et al.  Numerical Recipes: FORTRAN , 1988 .

[10]  A. Sinclair On the Origin of the Commensurabilities Amongst the Satellites of Saturn–II , 1972 .

[11]  Yoshihide Kozai,et al.  Secular perturbations of asteroids with high inclination and eccentricity , 1962 .

[12]  Dynamics and Origin of the 2:1 Orbital Resonances of the GJ 876 Planets , 2001, astro-ph/0108104.

[13]  C. Lousto,et al.  Three-body equations of motion in successive post-Newtonian approximations , 2007, 0710.5542.

[14]  P. Jaranowski,et al.  Radiative 3.5 post-Newtonian ADM Hamiltonian for many-body point-mass systems , 1997 .

[15]  B. Bruegmann,et al.  Characterization of the gravitational wave emission of three black holes , 2010, 1012.4423.

[16]  F. Rasio,et al.  RESONANCE TRAPPING IN PROTOPLANETARY DISKS. I. COPLANAR SYSTEMS , 2008, 0801.1926.

[17]  J. Makino,et al.  THE ORIGIN OF S-STARS AND A YOUNG STELLAR DISK: DISTRIBUTION OF DEBRIS STARS OF A SINKING STAR CLUSTER , 2010, 1003.4125.

[18]  A. Lemaitre,et al.  A second fundamental model for resonance , 1983 .

[19]  J. Schnittman THE LAGRANGE EQUILIBRIUM POINTS L4 AND L5 IN BLACK HOLE BINARY SYSTEM , 2010, 1006.0182.

[20]  N. Seto,et al.  Relativistic astrophysics with resonant multiple inspirals , 2010, 1005.3114.

[21]  P. Goldreich,et al.  An Explanation of the Frequent Occurrence of Commensurable Mean Motions in the Solar System , 1965 .

[22]  P. C. Peters Gravitational Radiation and the Motion of Two Point Masses , 1964 .

[23]  Fukun Liu,et al.  TIDAL STELLAR DISRUPTIONS BY MASSIVE BLACK HOLE PAIRS. II. DECAYING BINARIES , 2010, 1012.4466.

[24]  J. Lissauer,et al.  Resonant Inclination Excitation of Migrating Giant Planets , 2003, astro-ph/0308112.

[25]  John Asher Johnson,et al.  THE CALIFORNIA PLANET SURVEY. III. A POSSIBLE 2:1 RESONANCE IN THE EXOPLANETARY TRIPLE SYSTEM HD 37124 , 2011, 1101.1097.

[26]  Brett Gladman,et al.  Dynamics of Systems of Two Close Planets , 1993 .