|  Particle Dynamics in Schwarzschild Spacetime | 
Spinless Test Particles > s.a. classical particles;
  test-particle motion; schwarzschild geometry
  [line element, curvature].
  * Idea: Structureless particles
    in general relativity move along timelike geodesics of the metric.
  * Circular orbits: Test bodies
    can follow stable circular orbits at a radial distance r depending on
    their angular momentum, but always greater than 6R, where R
    is the Schwarzschild radius.
  * Precession: Non-circular orbits
    in Schwarzschild spacetime do not close, and are only approximately ellipses;
    With a quadrupole moment, the main contributions are δquadr
    = 6π (GM)Qm3/L4,
    and δgr
    = 6π (GM)2m2
    / L2c2, both positive.
  @ General references:
    in Weinberg 72;
    Wald 84, pp 140ff;
    Do-Nhat PLA(98);
    Dean AJP(99)jan [phase plane analysis];
    Mitra gq/99 [radial];
    Kerner et al CGQ(01)gq [nearly circular];
    Ajith et al PRD(05)gq/04 [post-Newtonian approximants];
    Boccaletti et al re GRG(05) [Beltrami's method];
    Hall a0807 [exact results];
    Brannen IJMPD(09)
      [Schwarzschild and Painlevé-Gullstrand coordinates];
    Hioe & Kuebel a1008 (comment
    Han a1008),
    a1010 [parametrized space of orbits];
    Bini et al CQG(11)-a1408 [non-geodesic orbits];
    Tsupko PRD(14)-a1505 [unbound trajectories, strong deflection].
  @ Null geodesics: Stuckey AJP(93)may;
    Čadež & Kostić PRD(05)gq/04;
    Belbruno & Pretorius CQG(11)-a1103 [dynamical-systems approach];
    Muñoz AJP(14)jun [exact solutions];
    Semerák ApJ(15)-a1412 [short formula];
    > s.a. geodesics.
  @ Other geodesics: Marck CQG(96)gq/95;
    Boccaletti et al GRG(05)gq;
    Leiva et al MPLA(09)-a0808 [in rainbow gravity];
    Scharf JModP(11)-a1101 [in terms of elliptic functions];
    Ohanian a1102
      [reversed gravitational acceleration for free fall motion at high speeds];
    Schmidt PRD(11)-a1104 [large eccentricity, perihelion advance];
    Kostić GRG(12)-a1201 [timelike, classification];
    Grib et al G&C(12)-a1203 [particle collisions];
    Tejeda & Rosswog MNRAS(13)-a1303 [accurate Newtonian description];
    Eufrasio et al GRG(18)-a1812;
    Ribeiro & Lima a1910 [timelike, exact solution].
  @ And gravitational radiation: Cardoso & Lemos PLB(02)gq.
  @ With radiation damping and radiation reaction: Burko PRD(03)gq/02;
    > s.a. orbits of gravitating bodies.
  @ Scattering: Mendoza et al Ent(09)gq/07 [absorption and reflection];
    Liu et al CQG(16)-a1512 [bending].
  @ Charged particles:
    Cardoso et al PRD(03)
  > Related topics:
    see gravitational self-force; sources
    of gravitational waves; Twin Paradox.
OIther Types of  Particles > s.a. chaotic
  motion in a curved spacetime; spinning particles.
  @ Spinning particles:
    Rietdijk & van Holten CQG(93);
    White et al CQG(00) [radial infall];
    Burko PRD(04)gq/03;
    Bini et al CQG(04)gq,
    CQG(05)gq [spin precession];
    Plyatsko CQG(05)gq [ultrarelativistic, circular orbits];
    Turakulov & Safonova MPLA(05) [s = 1, corrections to geodesics];
    Dolan et al PRD(06)gq [massive spin-1/2, scattering];
    Bini et al GRG(11)-a1408 [spin-geodesic deviations];
    Plyatsko & Fenyk PRD(12)-a1111;
    Jefremov et al PRD-a1503 [ISCO].
  @ Quadrupolar particles: Bini & Geralico PRD(13)-a1408.
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  send feedback and suggestions to bombelli at olemiss.edu – modified 13 oct 2019