In General > s.a. 3D gravity; causality
violation; singularities; solutions
with symmetries.
* The issue: M Choptuik,
in numerical simulations of spherically symmetric scalar field collapse, found
that, near the threshold for black-hole formation (criticality), the
mass of the black hole that forms always depends on the
parameter p in a family of initial data as
(p-pcrit)^
,
where
is
the same for all kinds of matter and initial conditions (universality);
The critical solution depended on r and t only
through the combination r/t (self-similarity).
* Development: Many other
studies, with different families of data and types of matter, numerical and
to some extent analytical, done since the
first
one; Universality may not be true [@ Maison PLB(96)gq/95].
Types of Matter and Theories > s.a. 3D
black holes.
@ Scalar: Hirschmann & Eardley PRD(95), PRD(95)gq [complex],
PRD(97)gq/95 [sigma
model]; Gundlach PRD(97)gq/96 [massless];
Hamadé & Stewart
CQG(96)gq/95 [massless];
Brady PRD(95),
et al PRD(97)gq,
Chambers et al gq/97-in
[massive, spherical]; Hod & Piran
PRD(97)
[charged]; Frolov PRD(00)gq/99 [continuous
to discrete self-similar]; Martín-García & Gundlach PRD(03)
[global structure]; Hirschmann
et al CQG(04)gq/02 [2+1];
Choptuik et al PRL(04)gq [complex,
with angular momentum].
@ 2+1, scalar + cosmological constant: Pretorius & Choptuik PRD(00) [numerical];
Husain & Olivier CQG(01); Garfinkle PRD(01) [exact]; Clément & Fabbri
CQG(01), NPB(02).
@ 2+1: Birmingham PRD(01)ht [BTZ
and AdS-cft]; Cavaglià et
al PRD(04)gq [
< 0
self-similar].
@ Higher-dimensional: Sorkin & Oren PRD(05)ht [massless
scalar]; Bizon et al PRL(05)
[4+1 vacuum]; Bland et al CQG(05)gq [scalar,
dimension dependence of critical exponent]; Bizon et al PRL(06)gq [5D
vacuum].
@ Dust: Singh & Joshi CQG(96); Joshi & Dwivedi CQG(99)gq/98 [spherical];
Olabarrieta gq/00-MSc.
@ Fluids: Maison PLB(96)gq/95 [non-universality];
Neilsen & Choptuik
CQG(00)gq/98;
Koike et al PRD(99); Carr e al PRD(00)gq/99,
CQG(01)gq/99;
Gundlach PRD(02)gq/99 [p = k
,
nonspherical]; Harada & Maeda PRD(01)gq [spherical]; Gundlach PRD(02)gq/01 [rotating].
@ Einstein-Yang-Mills: Choptuik et al PRL(96)gq,
PRD(99)gq;
Gundlach PRD(97)gq/96 [echoing
and scaling].
@ Newtonian gravity: Maeda & Harada PRD(01)gq;
Harada et al PRD(03)gq/02.
@ Other fields: Eardley et al PRD(95)gq [axion-dilaton];
Husa et al PRD(00)gq,
Thornburg et al gq/00-MG9
[
-model];
Ventrella & Choptuik
PRD(03)gq [Dirac]; > s.a. Sphaleron.
References > s.a. solar
system.
@ General: Choptuik PRL(93);
Abrahams & Evans GRG(94);
Aquilano et al GRG(94);
Husain et al PRD(94);
Das et al JMP(95);
Pürrer a0708-PhD
[global vs local aspects].
@ Reviews: Bizón ACosm(96)gq;
Choptuik gq/98-in;
Brady & Cai gq/98-in;
Gundlach ATMP(98)gq/97, LRR(99)gq/00,
PRP(03)gq/02;
Wang BJP(01)gq;
Hortacsu gq/03-in;
Gundlach & Martín-García LRR(07)-a0711.
@ Formulations: Garfinkle PRD(95)gq/94 [null];
Gundlach PRL(95)gq [eigenvalue
problem]; de Oliveira & Soares IJMPA(02)
[dynamical system]; > s.a. einstein's equation.
@ Renormalization approach: Hara et al gq/96;
Iguchi et al PRD(98)gq/97.
@ Self-similarity, scale invariance: Garfinkle & Meyer PRD(99);
Lechner et al PRD(02) [discrete/continuous bifurcation, sigma model].
@ Analytical models: Koike & Mishima PRD(95);
Husain et al CQG(96)gq/95;
Price & Pullin PRD(96)gq [approximations];
Wang PRD(03)gq [cylindrical
Klein-Gordon]; Mahajan & Joshi GRG(07)gq/05.
@ Perturbations: Frolov PRD(97)gq,
PRD(99)gq/98;
Gundlach PRD(98)gq/97 [non-spherical]; Garfinkle
et al PRD(99)gq/98 [angular
momentum]; Martín-García & Gundlach
PRD(99)gq/98 [non-spherical];
Garfinkle & Gundlach PRD(02)gq [2+1
+ scalar].
@ Related topics: Evans & Coleman PRL(94)
[radiation]; Pullin PLA(95)gq/94 [and
no-hair]; Gundlach PRD(98)gq/97 [angular momentum behavior]; Pürrer et
al PRD(05)gq/04 [radiation
and news].
@ Quantum: Strominger & Thorlacius PRL(94);
Tomimatsu PRD(95);
Brady & Ottewill PRD(98)gq;
Casadio gq/99-in
[shells]; Husain ASL(09)-a0808.
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send feedback and suggestions to bombelli at olemiss.edu – modified 9
aug 2009