The Program in General > s.a. canonical
general relativity and ADM formulation [classical
version].
* Idea: Geometrodynamics
is the program for canonical quantum gravity based on superspace and the dynamics
given there by the Wheeler-DeWitt equation;
A 4-geometry
is represented by a classical set of points C of superspace, contained
in
it as a hypersurface; The set of 3D geometries contains the time information;
Initial data consists of a neighborhood in C, from which the Einstein
equation gives C.
* Problems: Mainly interpretational, such as What is the meaning
of
(q,
)? We need an inner product for
's
before we say that |
|2 is a probability.
Kinematics: Superspace > s.a. canonical
quantum gravity; regge calculus [simplicial
superspace]; riemannian
geometry;
topology change.
* Idea: Superspace is a reduced configuration space for a Hamiltonian
formulation of gravity, in which a point is a diffeo equivalence class of Riemannian
metrics
on a spacelike hypersurface
: S(
):=
Riem(
)/Diff(
).
* Constraints: This choice
of configuration space eliminates the diffeomorphism constraint, but the scalar
one (coming from the gauge arbitrariness in choosing a slicing
of spacetime) remains, and becomes the dynamical equation.
* Topology: S(
)
is not a manifold, but is made up out of a finite number of manifolds (strata).
* Extended: Glue together
copies of the same space [@ DeWitt (70)].
* Grand: Need singular geometries.
* Minisuperspace: Impose
enough symmetries to get finite number of degrees of freedom.
@ Structure of superspace: & Peres < 79; Fischer in(70);
in Brill
in(72); Reula pr(GR12);
Christodoulakis & Zanelli pr(89); Giulini
HPA(95)gq/93, PRD(95)gq/93;
Fischer & Moncrief GRG(96)
[including conformal superspace]; Giulini GRG(09)-a0902.
@ Supermetric: Pekonen JGP(87);
Szydlowski JMP(99);
Schmidt gq/01-in.
@ Minisuperspace: Misner in(72); Kuchar & Ryan
in(86); Kiefer AP(91);
Kerbrat et al RPMP(92);
Saremi gq/01; > s.a. gowdy
spacetimes.
@ Related topics: Jacobson in(88) [self-dual representation]; Rainer gq/96-in
[locally homogeneous].
States: Wave Functionals > s.a. time
in quantum gravity.
* Idea: States are functionals
[qab,
]
of metrics (and matter fields) belonging to an appropriate space; Notice that
these states will end
up without
a time dependence, since they must satisfy the constraints; Instead,
time can be taken as one of the components of qab.
@ Inner product: DeWitt PR(67);
Tsamis & Woodard PRD(87);
Christodoulakis & Zanelli CQG(87);
Vilenkin PRD(89).
Dynamics: Wheeler-DeWitt Equation > s.a. 3D
quantum gravity; cosmological
constant; FRW models [solutions].
* Idea: The "zero-energy" Schrödinger-like
equation one gets as the operator version of the scalar constraint, by replacing q and p by
their coordinate representation operators (multiplication operator and –i
(
/
q),
respectively), and acting with it on a wave functional
[qab,
].
* Expression: For the dynamics of gravity coupled to a field
,
it is
![]()
up to linear derivative terms depending on the choice of factor ordering, where the supermetric, with "signature" (–,+,+,+,+,+) –the minus sign coming from the conformal mode– and thought of as a 6 × 6 matrix, is defined by
Gabcd =
q–1/2 (qac qbd
+ qad qbc – qab
qcd)
.
@ General references: Woodard CQG(93);
Jackiw gq/95 [modified];
Blaut & Kowalski-Glikman gq/96 [solutions,
and quantum potential]; Norbury EJP(98)phy [II,
from Newtonian physics]; Soo CQG(07)gq [in
terms of gauge-invariant 3-geometry elements]; Sawayama a0904 [small universe].
@ As spinor equation: Dereli et al PLB(94) [including degenerate metrics
and
signature change].
@ And stability of cosmological models: Gurzadyan & Kocharyan JETP(87);
Kocharyan
CMP(91).
References > s.a. canonical
quantum gravity; quantum cosmology [measure, third
quantization]; supergravity; supersymmetric
field theories.
@ General: Wheeler 62; Baierlein et al PR(62);
Fletcher in(62); Marzke & Wheeler
in(64);
Wheeler in(64); DeWitt PR(67);
Wheeler in(68); Wheeler 68; Brill & Gowdy
RPP(70);
DeWitt in(70); Fischer in(70);
Misner in(72); Christodoulou & Francaviglia AAST(76);
Shestakova a0801-in
[problems and approaches to their solution]; Kiefer GRG(09)-a0812 [overview].
@ Operator ordering: Hawking & Page NPB(86); Kontoleon & Wiltshire
PRD(99)gq/98;
Hall gq/04-in
[from "exact uncertainty"].
@ And time evolution: Kheyfets & Miller gq/94,
IJMPA(00);
Cosgrove
CQG(96)gq/95 [time
slicings and consistency]; Gil-Medrano
JMP(96);
Gentle et al IJMPA(04)gq/03,
George et al gq/03-in
[constraints and true degrees of freedom].
@ Relationships: Kubota et al PLB(04)
[Wheeler-DeWitt and AdS-cft].
@ WKB approximation: Gerlach PR(69); Horiguchi NCB(96).
@ Related topics: Parentani NPB(97)gq/96 [and
Green functions for matter fields];
Carroll gq/05 [uncertainties
and statistical geometrodynamics]; Nelson & Sakellariadou PLB(08)-a0709 [quantum
corrections
and effective matter]; Pedram & Jalalzadeh PRD(08)
[signature change with fluids]].
@ Generalizations: Shestakova G&C(99)gq/00,
G&C(05)
[extended
phase space],
G&C(00)gq [and
cosmological constant], a0810-in;
Belinchón
IJMPD(02)gq/01 [varying
constants]; > s.a. phenomenology [with non-linear correction].
main page – abbreviations – journals – comments – other
sites – acknowledgements
send feedback and suggestions to bombelli at olemiss.edu – modified 24
apr 2009