In General > s.a. differential
geometry [completeness]; group
action [actions
preserving geodesics].
$ Def: A geodesic is a curve in a manifold whose tangent vector X is parallel to itself along the curve, or
X X
= f X , for some function f .
* Affine parametrization:
It is always possible to parametrize a geodesic such that
X X =
0; This is equivalent to
d2xm/dt2 +
mpq
(dxp/dt) (dxq/dt) =
0 .
* As extremal curves: If the connection is torsionless, geodesics
extremize the distance between two points.
* Properties: The geodesics
of a manifold depend on the metric, but are
insensitive to its torsion, as can be seen from above; For an affinely parametrized
geodesic, the
norm of the tangent vector is constant along it.
@ General references: Busemann 55; in Arnold 89, app1 [concise];
Boccaletti et al GRG(05)gq [Beltrami
method + Schwarzschild and Kerr].
@ Conformal
geodesics:
Friedrich & Schmidt PRS(87); Friedrich CMP(03)gq/02.
@ Quantum corrections: Dalvit & Mazzitelli gq/99-in,
PRD(99)gq.
Geodesic Deviation and Focusing > s.a. regge
calculus; torsion.
$ Def: If Xa:=
xa/
s is
the connecting vector between nearby
geodesics
in a one-parameter family, and T a:=
xa/
t the
tangent
vector,
the
relative acceleration
aa:= D2Xa/Dt2 = Rabcd T b T c X d .
* Jacobi equation: The
linearized equation for a particle (or a field theory) around an extremal of
the action; Used for the linearized geodesic flow, it
gives the
geodesic deviation equation; A Jacobi field is a solution of the Jacobi
equation,
i.e., a linearized solution of the equations of motion.
@ General references: Barraco et al GRG(90);
Roberts GRG(96)gq/99 [from
action, quantization]; Kerner et al
PRD(01)gq/00 [in
Kaluza-Klein]; Colistete et al CQG(02)
[higher-order, in Kerr].
@ Jacobi equation: Núñez-Yépez & Salas-Brito
PLA(00)mp [variational
principle]; Chicone & Mashhoon CQG(02)gq,
Perlick GRG(08)-a0710
[generalized].
@ Geodesic focusing: in Hawking in(73) [simple intro]; O'Sullivan MA(74);
Rosquist
IJTP(83);
Visser PRD(93)
[Lorentzian spacetime]; Ehlers & Newman
JMP(00)gq/99 [caustics].
Related Notions > see Congruence and
Congruence Expansion; Totally
Geodesic [mapping, submanifold].
* Maslov
index: For a semi-Riemannian geodesic, a homological invariant which
substitutes the notion of geometric index in Riemannian geometry.
@ Geodesic flow as dynamical system: Hedlund BAMS(39); > s.a. conserved
quantities.
@ Other references: Rotman Top(07)
[length of minimal geodesic net on
a closed Riemannian manifold]; Bolsinov et al a0806 [Fubini theorem, for pseudo-Riemannian
metrics].
> Space of geodesics: see symplectic structure.
Null Geodesics > s.a. coordinates [based on a null geodesic].
* Set of
null geodesics: If (M, g) is a globally
hyperbolic
(d+1)-dimensional
spacetime, this set
is
naturally a smooth (2d–1)-dimensional contact manifold.
* Sky: The sky of an event is
the subset of
defined
by all
null
geodesics through that event, and is an embedded Legendrian submanifold
of
diffeomorphic to a Sd–1.
@ General references: Low JMP(89);
Urbantke JMP(89);
Frittelli & Newman gq/98-in
[time of arrival].
@ Types of spacetimes: Frittelli et al CQG(98)
[asymptotically flat, conjugate points];
Stuckey AJP(93),
Cadez & Kostic
PRD(05)gq/04 [in
Schwarzschild spacetime]; Hall & Lonie JMP(08)
[FRW spacetimes].
@ Properties of skies: Natário CQG(02)gq/01 [skies];
Natário & Tod PLMS(04)gq/02.
Types of Spaces > s.a. connections [non-commutative]; solutions
with symmetries [static];
graph theory; regge
calculus.
@ 2D:
Knieper & Weiss JDG(94) [S2, positive topological
entropy]; Lévay JPA(00),
JPA(00)
[negative curvature Riemann surfaces]; Rowland EJP(06)
[simple]; Ying & Candès JCP(06) [computation].
@ Riemannian: Berger 65; Bolsinov & Jovanovic in(04)mp/03
[integrability].
@ Lorentzian: Larsen JDG(96)
[sic];
Candela & Sánchez m.DG/06 [rev].
@ Bianchi metrics: Nilsson et al GRG(00)gq/99 =
GRG(00)
[dynamical
system]; Valent & Yahia CQG(07)
[integrable flows]; > s.a. bianchi models.
@ Black hole spacetimes: Marck CQG(96)gq/95 [Schwarzschild-Kerr];
Leiva
et al MPLA(09)-a0808 [Schwarzschild
metrics in rainbow gravity]; Slany et al IJMPA(09)
[Kerr-de Sitter]; > s.a. kerr
spacetimes.
@ Other metrics: Moraes PLA(96)
[dislocation]; Barrow & Levin PLA(97)
[k = –1 FRW models]; Podolsky & Belán CQG(04)
[Kundt spacetimes]; Herrera FPL(05)
[quash-spherical]; D'Afonseca et al CQG(05)gq
[Weyl-Bach ring solution]; Kiosak & Matveev CMP(09)-a0806 [geodesically
rigid]; Brink PRD(08)-a0807 [stationary
axisymmetric vacuum]; > s.a. FRW
metrics; Lemaître-Tolman-Bondi, Lewis
Metric, test-particle motion.
Physics Applications > s.a. de
Sitter-Fokker Precession; jacobi dynamics; particle
models; perfect fluids;
Sachs-Wolfe Effect.
* Main application: Paths
of test
particles in curved spaces; > s.a.
chaos,
general relativistic chaos.
* Multiple imaging: The local geometry equivalent of "gravitational
lensing," weaker
than focusing.
@ References: Kuusk & Paal TTTU(92)-a0803 [geodesic
multiplication, Akivis algebras]; Perlick CQG(96)
[multiple imaging]; Adamo et al LRR(09)-a0906 [asymptotically
shear-free null geodesic congruences].
> In gravitation and cosmology:
see geometrodynamics; cosmological
models
in general relativity [dynamics as geodesic motion]; motion
of
gravitating
bodies.
main page – abbreviations – journals – comments – other
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send feedback and suggestions to bombelli at olemiss.edu – modified 13
sep 2009