ADM Formulation of General Relativity  

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

qabeab = O(r–1) ;   c qab & Kab = O(r–2) ;   cd 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 'abh'ab ab) dv .

* Constraints and Hamiltonian:

:= q1/2 3R q–1/2 (pabpab p2) ,   b:= Da pab ,   H = Sigma d3x (N + Naa) .

* Constraint algebra: If the smeared scalar and vector constraints are, respectively [f] = Sigma d3x f and [f a] = Sigma d3x f aa, then

{[f a], [ga]} = [f ga] ;     {[f a], [g]} = –[f g] ;     {[f], [g]} = –[qab (fb ggb 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 = (16G)–1 limr to infty (a qbcb qac) eac dS b
pm = (8G)–1 limr to infty (KabKcc qab) Na dS b = (8G)–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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