In General > s.a. [computational
physics, numerical
relativity]; actions for general relativity;
quantum
regge calculus.
* Idea: A way of doing
calculations in a discretized manifold; Initially the simplex version was
used, then 3+1 and continuous-time versions developed,
which were thought to be more useful for evolution questions and canonical
quantization.
* Applications: The main
one is as a tool in numerical relativity, related to the finite element method;
Results usually agree well with continuum
ones,
except when a bounce occurs in collapse (1991).
* Variables: The metric
for an n-dimensional
manifold is given by assigning the lengths (squared) of all sides of all simplices;
This gives, for each simplex, n(n+1)/2 parameters (ok with
counting of metric components); The kinds of metrics that can be given in this
way are limited, because if
one
imagines the simplexes as superimposed on a smooth manifold, "all the
curvature" is
contracted at discrete points: the rest is flat.
* Hilbert-Einstein action: Can be expressed (up to some coefficient)
by the exact formula
R dv =
i
(i) A(i)
,
where the summation is over all (n–2)-simplexes i,
of area A(i) (with A(i):=1 if n–2
= 0), and the defect angle
is
by
(i):=
2
–
_{
i}
(i;
),
(i;
)
being the angle of
the (n–1)-simplex
at i.
References
@ General: Regge NC(61); in Wheeler in(64); in
Misner et al 73 [clear; good introduction]; Williams NS(86)
[I].
@ Action: Lund & Regge pr(74); Hartle & Sorkin GRG(81)
[boundary terms]; Piran & Williams PRD(86);
Brewin CQG(88);
Miller CQG(97)gq;
Khatsymovsky a0804 [Holst action, Immirzi parameter].
@ And general relativity: Cheeger et al in(82), CMP(84);
Friedberg & Lee NPB(84);
Barrett CQG(87), & Parker
pr(90); Brewin GRG(89), & Gentle
CQG(01)gq/00;
Kemmell IJTP(94);
Chakrabarti et al CQG(99)gq/98 [geodesic
deviation].
@ Continuum limit: Ôgami CQG(97)
[2D action]; Khatsymovsky PLB(02)gq [area
variables]; Bittner et al hl/03-in.
@ Initial value problem: Sorkin PRD(75);
Piran & Williams PRD(86);
Porter CQG(87); Barrett
et al IJTP(97)gq/94 [parallelizable].
@ Simple spaces and formulae: Hartle JMP(85), JMP(86); Piran & Strominger
CQG(86).
@ Bianchi identities: in Regge NC(61); in
Miller FP(86);
Bezerra CQG(88);
Hamber & Kagel
CQG(04)gq/01.
@ Geometry: Williams & Ellis GRG(81)
[geodesics]; Brewin CQG(88)
[Riemann and extrinsic curvature], PRD(88)
[trapped
surface]; McDonald & Miller a0804-in,
a0805-CQG
[dual tessellations and scalar curvature].
@ Affine tensor and exterior calculus: Warner PRS(82); Brewin JMP(86).
@ Related topics: Rocek & Williams in(82) [conformal transformations];
Hamber & Williams NPB(97)ht/96 [gauge invariance].
Various Versions > s.a. discrete
geometries; dynamical
triangulations; lattice gravity.
* Regge approach: Fix
the triangulation and vary edge lengths; Typically use R2 actions
(bouded below) or the EH action.
* Canonical: 1991, There
is a problem with the closing of the constraint
algebra.
* Discrete time: Foliate
spacetime into hypersurfaces (e.g., spacelike), divide each one into convenient
blocks in the same
way (e.g., by simplices), then join
corresponding
vertices by edges (obtaining a total tessellation by prisms).
* Null strut calculus:
Build simplicial spacetimes with the maximal number of null edges; This reduces
the number of variables and simplifies one type of equation, which becomes
a linear
relation between deficit angles.
@ Regge approach: Hamber PRD(92)
[phase transition]; Brewin CQG(98)gq/97 [different
implementation of Einstein equation].
@ Canonical, constraints: Friedman & Jack JMP(86);
Khatsymovsky CQG(94)gq/93; Mäkelä PRD(94);
Tuckey & Williams CQG(90);
Bander PRD(87)
[d-dimensional, constraint algebra]; Khatsymovsky GRG(95)gq/93, PLB(00)gq/99;
Gambini & Pullin IJMPD(06)
[and consistent discretization].
@ Tetrad/Ashtekar version: Khatsymovsky CQG(89), CQG(91),
gq/93;
Immirzi CQG(94)gq.
@ Discrete time: Porter PhD(82); Brewin PhD(83), CQG(87);
Dubal PhD(87); Tuckey CQG(89), CQG(93)gq.
@ Null strut calculus: Miller & Wheeler NC(85);
Miller PhD(86); Kheyfets
et al PRL(88),
CQG(89),
PRD(90),
PRD(90).
@ Area variables: Barrett et al CQG(99)gq/97;
Mäkelä CQG(00)gq/98, & Williams
CQG(01)gq/00;
Wainwright & Williams CQG(04)gq [and
discontinuous
metrics]; Dittrich & Speziale a0802 [area-angle variables].
@ First-order form: Barrett CQG(94)ht;
Gionti gq/98.
@ Variations: Barrett PLB(87), CQG(88)
[linearized]; Brewin PRD(89)
[ADM 4-momentum];
Reisenberger CQG(97)gq/96 [left-handed];
Bilke et al PLB(98)hl/97 [U(1)
fields];
Schmidt & Kohler GRG(01)gq [dislocations
and torsion].
Types of Spacetimes > s.a. FRW
spacetime; bianchi
I [Kasner]; quantum regge calculus.
@ 2D: Beirl & Berg
NPB(95)hl;
Hamber & Williams NPB(95);
Hartle & Perjés JMP(97)gq/96 [CP2];
Rolf ht/98-PhD
[quantum].
@ 2D, random
triangulations: Holm & Janke PLB(97)hl/96;
Carfora et al CQG(02)gq.
@ 3D: Rocek & Williams CQG(85); Boulatov & Krzywicki MPLA(91);
Boulatov
JHEP(98).
@ 3D, Topics: Waelbroeck CQG(90)
[constraints]; Durhuus & Jonsson
NPB(95)
[entropy]; Hartle et al CQG(97)gq/96 [simplicial
superspace].
@ Schwarzschild: Brewin CQG(93); Williams & Ellis GRG(84).
@ Taub universe: Tuckey & Williams CQG(88) [3+1, continuous time].
@ Other types: Collins & Williams PRD(74)
[Tolman]; Porter CQG(87)
[spherical symmetry], CQG(87)
[model stars]; Dubal CQG(89)
[radiation], CQG(89), CQG(90)
[collapse]; Clarke et al CQG(90)
[cosmic strings]; Bilke et al PLB(97)
[topology and free energy]; Gentle CQG(99)
[Brill waves,
initial data];
Khatsymovsky PLB(00)gq/99,
PLB(00)gq/99 [simple
model, path integral and canonical], PLB(03)gq [discontinuous].
Other References > s.a. higher-order
gravity; numerical general relativity;
quantum spacetime.
@ Geometrical aspects: Caselle et al PLB(89)
[dual lattice]; Miller FP(86);
Jourjine PRD(87)
[ito cell complex]; Brewin CQG(88).
@ Intros, reviews: Williams & Tuckey CQG(92); Immirzi NPPS(97)gq [comments];
Gentle & Miller gq/01-MG9;
Regge & Williams JMP(00)gq;
Gentle
GRG(02)gq/04 [numerical
relativity]; Larrañaga gq/03-ln
[en español].
@ Convergence, consistency: Brewin gq/95;
Miller CQG(95)gq; Brewin GRG(00).
@ Scaling, renormalization: Martellini & Marzuoli in(86); Mitter & Scoppola
CMP(00)ht/98; Hamber
PRD(00)ht/99.
@ And matter: Weingarten JMP(77)
[electromagnetism]; Berg et al PRD(96)
[SU(2) gauge theory]; Khatsymovsky PLB(01)gq/00;
Bittner et al PRD(02)
[Ising spins].
@ For similar theories: Sorkin PhD(74), JMP(75)
[electromagnetism]; Pereira & Vargas
CQG(02)gq [teleparallel gravity].
@ Gauge theory style: Weingarten NPB(82); Kawamoto & Nielsen PRD(91).
@ Entropy: Ambjørn & Varsted PLB(91); Bartocci et al JGP(96)ht/94;
Carfora & Marzuoli JGP(95).
@ (No) exponential bound, thermodynamic limit: Ambjørn & Jurkiewicz PLB(94);
Catterall
et al PRL(94);
Carfora & Marzuoli
JMP(95).
@ Random simplices: Ambjørn et al NPB(93) [Euclidean]; David
in(95)ht/93;
Carfora et al gq/03-in
[2D].
@ Random surfaces: Kostov & Krzywicki PLB(87); Polyakov 87; Ambjørn
NPPS(95)hl/94,
et al 97; Thorleifsson NPPS(99)hl/98.
@ Random/polymerized manifolds: Gabrielli PLB(98);
Harris & Wheater PLB(99)ht/98.
@ Phase structure: Hamber
PRD(92);
Catterall et al PLB(94).
Main page – Abbreviations – Journals – Comments – Other
sites – Acknowledgements
Send feedback and suggestions to bombelli at olemiss.edu – Modified
5 jul 2008