|  Reissner-Nordström Spacetimes | 
In General > s.a. black holes;
  generalized reissner-nordström spacetimes.
  > Note: The spelling is
    Reissner-Nordström, not Reissner-Nordstrøm [@ see Brill &
    Dray GRG(93)].
  $ Def: A family of solutions
    of Einstein's equation representing a non-rotating black hole with non-zero
    electric charge, depending on the parameters M (mass) and Q
    = (Qe2
    + Qm2)1/2
    (electromagnetic charges) [c = 1], and line element
ds2 = −(1 − 2GM/r + GQ2 /r2) dt2 + (1 − 2GM/r + GQ2 /r2)−1 dr2 + r2 dΩ2 .
  * Singularities:
    For Q2 > GM2,
    we get a naked singularity; For Q2 <
    GM2, a regular black-hole solution with
    two horizons, at r = r±
    = GM ± (G2M2
    − GQ2)1/2
    (from grr = 0), besides the true
    singularity at r = 0; For Q2
    = GM2, the extreme case.
  * Electromagnetic field:
if Qm = 0, Aa = (Qe/r, 0, 0, 0), F01 = −Qe/r2 ; if Qe = 0, Aa = (0, −Qm sin θ, 0, 0), F23 Qmsin θ .
  * Symmetries: The only conformal
    or projective vector fields it admits are its standard Killing vector fields [@ Hall
    CQG(00)].
  * Fermat geometry:
    For P = 0, if q:= Q/M and
    d2:= 1−q2
    (the horizon is at r/M = 1/d), then the Fermat geometry is non-hyperbolic
    for r/M > 1 + (d/2)2/3; One can get
    arbitrarily close to the horizon (> SS 1.12.1995).
  @ General references:
    Reissner AdP(16);
    Nordström PKNAW(18);
    Klösch & Strobl CQG(96) [global coordinates];
    Marsh FP(08)-a0708;
    Riazuelo IJMPD(19)-a1812.
  @ Singularities: Giveon et al JHEP(04)ht [resolution, with scalar fields];
    Abdel-Megied  & Gad CSF(05)gq/04;
    Stoica PS(12)-a1111 [extension];
    Chesler et al a1902 [from charged scalar field collapse];
    > s.a. perturbations [without singularities].
  > Online resources:
    see Wikipedia page.
Special Topics
  > s.a. black-hole entropy; particle models;
  perturbations [including stability]; spherical
  symmetry; thermodynamics [including phase transitions].
  @ Interior: Bonanno et al PRS(95)gq/94 [mass inflation];
    Ivanov PRD(02)gq [pfluid];
    Lemos & Zanchin PRD(11)-a1104 [de Sitter];
    Hansraj et al IJTP(14).
  @ Mass: Hushwater gq/01-wd;
    Barbachoux et al IJMPD(02)gq;
    Herrera et al GRG(03)gq [active mg].
  @ The extremal limit: Wang et al PRD(98)gq [no-go for physical process];
    Carroll et al JHEP(09)-a0901 [discontinuous nature, and black-hole entropy].
  @ Embeddings: Paranjape & Dadhich GRG(04)gq/03 [embedding diagrams];
    Paston & Sheykin Sigma(14)-a1304 [global embeddings in flat space].
  @ Foliations: Reimann & Brügmann PRD(04)gq [maximal slicing, late time];
    Qadir et al NCB(07) [K-slicing];
    Tuite & Ó Murchadha a1307 [constant-mean-curvature slices].
  @ Other related topics:
    Couch & Torrence GRG(84) [spatial inversion];
    Abramowicz et al CQG(02)gq [Fermat/optical geometry];
    Chen & Sun JHEP(10) [hidden conformal symmetry];
    Bengtsson et al CQG(14)-a1406 [the \(Q\to0\) and \(Q\to M\) limits];
    Crispino et al EPJC-a1602 [tidal forces].
Motion of Particles and Waves
  > s.a. klein-gordon fields; lensing;
  matter near black holes; types of geodesics.
  @ Particles: Dean GRG(99) [orbit precession];
    Pradhan & Majumdar PLA(11)-a1001 [extremal, ISCOs];
    Pugliese et al a1003-MG12 [circular motion];
    Misra & Levin PRD(10)-a1007 [taxonomy of orbits];
    Grunau & Kagramanova PRD(11)-a1011 [charged particles];
    Pugliese et al PRD(11)-a1012 [neutral particles, circular geodesics],
    PRD(11)-a1103,
    EPJC(17)-a1304 [charged particles];
    Pradhan Pra(16)-a1205,
    Pugliese et al EPJC(17)-a1304 [circular orbits];
    Das et al a1609 [charged particles, Jacobi metric approach];
    Hong a1709 [test particles].
  @ Spinning particles: Ali & Ahmed AP(00);
    Mukhopadhyay CQG(00) [spin-1/2, charged];
    Bini et al PRD(00),
    IJMPD(05)-a1408;
    Firsova MPLA(03) [scattering].
  @ Scalar fields: Ori PRD(98)gq/97 [massless];
    Wang & Huang PRD(01) [back-reaction];
    Sini & Kuriakose IJMPD(09)-a0708 [WKB approximation];
    Babichev et al JETP(11)-a0806 [and perfect fluid];
    Matyjasek et al PRD(10)-a1005 [quantum, vacuum polarization];
    Aretakis a1006 [wave equation on extreme solution];
    Chen & Jing PRD(10)-a1007;
    Dain & Dotti CQG(13) [wave equation on the extreme Reissner-Nordström solution];
    Franzen a1407 [boundedness in the interior].
  @ Electromagnetic fields:
    Torres del Castillo & Cartas-Fuentevilla PRD(96) [and gravitational waves];
    Crispino & Oliveira PRD(08),
    Crispino et al PRD(09) [absorption cross section].
  @ Other fields: Goncharov PLB(99)gq [twisted spinors];
    > s.a. dirac fields in curved spacetime.
  @ Wave tails:
    Koyama & Tomimatsu PRD(01) [massive scalar];
    Blaksley & Burko PRD(07)-a0710 [same as in Schwarzschild spacetime].
 main page
  – abbreviations
  – journals – comments
  – other sites – acknowledgements
  send feedback and suggestions to bombelli at olemiss.edu – modified 30 nov 2019