In General > s.a. quantum
black holes; spherical solutions; schwarzschild
geometry [line element, curvature].
* Idea: The first solution
(other than Minkowski space) in general relativity, found in 1916, and one
of the most important, equivalent to the Kepler problem in
classical mechanics;
The 1-parameter family of static, spherically symmetric vacuum solutions,
representing
black holes.
@ General references: Schwarzschild VAG(00)-CQG(98), SPAW(16)-GRG(03)phy/99,
SPAW(16)phy/99;
in Hawking & Ellis 73; in Wald 84; Gruber
et al AJP(88)
[derivation no-go]; Santander et al AJP(97)
[curvature-based]; Visser IJMPD(05)gq/03 [heuristic];
Antoci phy/03-in,
Gsponer phy/04 [history];
Deser & Franklin AJP(05)gq/04 [derivation];
Schmidt GRG(05)gq/04 [Synge's
contribution]; Bel a0709.
@ Characterization: Ferrando & Sáez CQG(98);
Fernández-López
et al JGP(03).
@ Geometry: Kling & Newman PRD(99)
[null cones]; Rama PLB(04) [ito branes and antibranes].
> Other: see Birkhoff's
Theorem; perturbations.
Specific Concepts > s.a. Irreducible
Mass; lensing; schwarzschild
geometry; yang-mills
gauge theory.
* Singularities:
=
0,
, removable (use Cartesian-like
coord's);
r = 2GM, removable; r = 0, curvature singularity.
@ Singularity: Hellaby JMP(96); Heinzle & Steinbauer JMP(02)gq/01 [distributional]; > s.a. types
of singularities.
@ Boosted (Aichelburg-Sexl): Barrabès & Hogan PRD(01)gq; > s.a.
solutions of general relativity.
@ Interior: Som et al PLA(01)
[matter]; Füzfa et al GRG(02)
[Lemaître-Schwarzschild]; Doran
et al FP(08)gq/06; > s.a.
black holes.
@ Extensions: Frønsdal PR(58); Rosen AP(71); Klösch & Strobl
CQG(96); Mitra ap/99 [??];
Abbassi PS(01)gq/99.
@ Canonical approach: Varadarajan PRD(01)gq/00 [Kruskal
variables].
@ Quantum corrections: Becker & Becker PRD(99)
[11D matrix theory]; Vaz & Witten PRD(99)gq/98 [canonical];
Buric & Radovanovic CQG(00);
Cavaglià & Ungarelli
PRD(00)ht/99 [mass];
Cavaglià & Fabbri PRD(02)ht/01 [AdS2 and n-Schwarzschild];
Bjerrum-Bohr
et al PRD(03)ht/02 [and
Kerr]; Khriplovich & Kirilin JETP(04);
Fabbri et al ht/05-in;
Kirilin
gq/06; Holstein
gq/06 [spin-1,
and Kerr]; > s.a. black hole entropy, covariant
quantum gravity, semiclassical general relativity.
@ With matter: Hartle in(72) [long-range neutrino forces]; Goncharov PLB(99)gq [twisted
spinors]; Molnár & Elsässer
PRD(03)gq [uniqueness
of electrostatic solution]; Bormann & Antonsen IJTP(04)
[0-pt energy, scalar
and
fermion fields]; Doran et al PRD(05)
[fermion absorption cross section]; Sharif & Sheikh GRG(07)-a0705
[cold plasma, dispersion
relations].
@ Other: Abrams CJP(89)gq/01 [??];
Quirós gq/99 [spurious??];
Nikishov
gq/00 [energy-momentum
pseudotensor]; Krasnov & Solodukhin ATMP(04)ht [stringy
description]; Antoci & Liebscher gq/04-in
[surface is singular??].
> With matter: see black
hole
phenomenology; classical particles; spinning
particles; test particles; waves
and
fields.
> Related topics: see
geodesics; green functions; metric
matching; perturbations;
Phantom Field; self-force; Weyl-Lanczos
Equations.
> Other: see boundaries [extensions?]; cosmic
strings; regge
calculus; sources of gravitational waves.
In Cosmological Backgrounds > s.a. FRW
spacetimes; reissner-nordström; schwarzschild-de
sitter.
* Idea: Solutions which
represent a black hole or local system in an asymptotically FRW spacetime,
or other cosmological background.
* McVittie solution: The k =
0 line element in Hogan's form is

where M
"mass
at the singularity," and
(t)
(asymptotic) expansion rate.
* Relationships: McVittie
becomes FRW for r →
,
Schwarzschild for d
/dt =
0, Schw-dS for d2
/dt2 =
0.
@ McVittie solution: McVittie MNRAS(33);
Newman & McVittie GRG(82)
[many particles]; Hogan ApJ(90); Nolan PRD(98)gq,
CQG(99), CQG(99)gq;
Patel et al G&C(00)
[higher-dimensional]; Bolen et al CQG(01)gq/00 [precession].
@ Schwarzschild-FRW solutions: Gautreau PRD(84);
Grøn & Rippis
GRG(03)gq;
Gao CQG(04) [arbitrary D].
@ In other backgrounds: Nayak et al PRD(01) [Einstein universe].
Other Similar Solutions > s.a. black
hole solutions; branes; dilaton
gravity;
gravitational instanton [Euclidean]; kerr.
* Conformal gravity:
Replace 1 – (2GM/r)
1 – (2GM/r)
+
r – kr2 in
line element above (
, k integration
constants).
@ Non-commutative:
Nasseri GRG(05)ht,
comment Li ht/05;
Nicolini et al PLB(06)gq/05 [and
evaporation]; Nasseri IJMPD(06).
@ Other theories: Federbush gq/00 [quadratic
curvature]; Zet gq/03 [teleparallel
gravity with torsion].
@ Other: Abrams PRD(79)gq/02 [Droste-Weyl-Schwarzschild];
Dadhich et al Pra(98)gq/97 [with
global monopole charge]; Aichelburg & Balasin
CQG(98),
CQG(00)
[ultrarelativistic]; Gen & Shiromizu JMP(99)
[asymptotically Schwarzschild];
Ren & Lichun NCB(01) [sourrounded by radiation];
de Felice & Sorge CQG(03)
[with magnetic field, orbits]; Martínez-Morales gq/05;
Al-Badawi
& Halilsoy GRG(06)
[+ Robinson-Bertotti, and NUT parameter]; > s.a.
holonomy [Schwarzschild-Droste]; modified
black hole solutions;
perturbations [including negative M].
Main page – Abbreviations – Journals – Comments – Other
sites – Acknowledgements
Send feedback and suggestions to bombelli at olemiss.edu – Modified
20 jun 2008