In General > s.a. 3D gravity; fluids;
initial-value formulation; lattice
gravity; metric decomposition; numerical
relativity.
$ Variables: Phase space is
the set of pairs (qab, pab), where qab is a
positive-definite metric on
and pab a
tensor density of weight 1, related to the extrinsic curvature Kab (in
a solution) by
pab = (q1/2/2
) (Kab – Kqab) , or Kab
= 2
q–1/2(pab –
pqab)
.
* Boundary conditions:
The spacetime (M, gab)
is asymptotically flat at spatial infinity if the data (qab, Kab)
induced on a spacelike hypersurface
are
such that
qab – eab = O(r–1)
;
c qab & Kab = O(r–2)
;
c
d qab &
cKab = O(r–3); etc
;
One can then find a chart such that qab =
(1 + M/2r)4 eab + O(r–2);
In covariant form, gab =
ab +
ab,
ab = O(
–1)
in the Cartesian chart for
.
* Symplectic structure:
|(q,
p)[(h,
),
(h',
')]
=
Sigma (hab
'ab – h'ab
ab)
dv .
* Constraints and Hamiltonian:
:= q1/2 3R – q–1/2 (pabpab –
p2)
,
b:= Da pab , H =
Sigma d3x (N
+
Na
a)
.
* Constraint algebra: If
the smeared scalar and vector constraints are, respectively
[f]
=
Sigma d3x f
and
[f a]
=
Sigma d3x f a
a,
then
{
[f a],
[ga]}
=
[
f ga]
; {
[f a],
[g]} = –
[
f g]
; {
[f],
[g]} = –
[qab (f
b g – g
b f]
.
@ General articles: Dirac PRS(58), PR(59);
Arnowitt et al JMP(60), PR(60),
in(62) [+ GRG(08)];
Anderson RMP(64);
Kuchar JMP(72)
[bubble-time formalism]; Regge & Teitelboim AP(74)
[boundary terms]; Isenberg & Nester
in(80); Ashtekar PhyA(84)
[good summary]; Beig & O'Murchadha AP(87)
[boundary conditions]; Grishchuk & Petrov JETP(87);
Vulcanov & Ciobanu AUVT(01)gq/00 [Maple
routines]; Brewin PRD(09)-a0903 [equations
from second variation of arclength].
@ Constraint algebra: Teitelboim AP(73);
Kouletsis CQG(96)gq;
Markopoulou CQG(96)gq; > s.a. constraints.
@ Embedding variables: Hojman et al AP(76);
Kuchar JMP(76);
Isham & Kuchar AP(85);
Braham JMP(93);
Ambrus & Hájícek PRD(01)gq/00 [relationship
with ADM]; > s.a. models in canonical general relativity [shells].
Energy-Momentum > s.a. canonical general
relativity; angular
momentum.
$ Def: Given a spacelike
surface
in
spacetime which is asymptotically flat at spatial infinity, with induced metric qab
and a reference flat metric eab,
the ADM four-momentum associated
with it is defined by
E = (16
G)–1 limr to
infty
(
a qbc –
b qac) eac
dS b
pm = (8
G)–1 limr to
infty
(Kab– Kcc qab) Na dS b =
(8
G)–1 limr to
infty
pab Na
dS b,
where r2 =
i (xi)2,
with x1, x2, x3 asymptotically
Euclidean coordinates for eab,
the integrals are taken over constant r spheres,
and N is an asymptotic translation; The results are independent of
the choice of eab, and
the vector Pa = –Ena+pa
is independent of S (i.e.,
it is conserved), where na is
the future-directed unit timelike
normal to
at spacelike
infinity.
@ Asymptotically flat: Arnowitt et al PR(59), PR(60),
PR(61),
in(62); Ashtekar & Horowitz PLA(82)
[cannot be null]; Baskaran et al AP(03)gq [relationships];
Shi & Tam m.DG/04 [mass
estimates]; Brewin GRG(07)gq/06 [simple
mass expression].
@ More general spacetimes: Nucamendi & Sudarsky CQG(97)gq/96 [quasi-asymptotically
flat].
Variations > s.a. 3D general relativity; non-standard
approaches to canonical general relativity.
@ Various theories: York gq/98;
Menotti & Seminara AP(00)ht/99, ht/99-in
[2+1 with particles]; Barbashov et al IJMPA(08)ap/05-in;
Lacquaniti & Montani IJMPD(06)gq,
gq/06-in [5D
Kaluza-Klein]; Chakrabarti et al a0908 [f(R) gravity].
@ Extended objects:
Capovilla et al NPPS(00)ht;
Steinhoff et al PRD(08),
Steinhoff & Schäfer EPL(09)-a0907 [spinning
objects].
@ Null surfaces: Goldberg in(86), pr(86); Torre CQG(86); Goldberg et al
CQG(92).
@ Other theories and variations: Gunnarsen CQG(89)
[weak field]; Brown & Marolf PRD(96)gq/95 [material
reference systems]; Watson & Klauder CQG(02)gq/01 [metric
on phase space]; Bonanno et al
CQG(04)gq [variable G and
];
Wang PRD(05)gq [conformal];
Brown a0802 [strongly
hyperbolic extension]; Ghalati a0901; > s.a. modified general
relativity; numerical
relativity [BSSN
form].
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oct 2009