Topics, S
S Theorem > see lie algebra.
S-Matrix > s.a. [quantum
field theory techniques]; Coleman-Mandula
Theorem; LSZ
Formalism.
* History: Introduced
by J Wheeler in the context of nuclear physics.
$ Def: In quantum field
theory, the operator S:=
lim U(t, t0)
for t →
, t0 → –
,
where U is
the time evolution operator.
* Assumptions: Causality, unitarity, analiticity.
* Properties: Its unitarity,
to first order, is (formally) equivalent to conservation of probability; To
second order it is guaranteed by completeness
of the Hilbert space and self-adjointness of the (interaction) Hamiltonian.
* Transition matrix: The matrix T related to the S-matrix by Sfi =
fi –
2
i
(
f –
i)
Tfi.
@ References: Stern PT(64) [criticism];
White hp/00-in
[review]; Kummer EPJC(01)ht [gauge
invariance]; Colosi & Oeckl a0710 [new approach].
Sachs-Wolfe Effect > see CMB anisotropies.
Saddle-Point Approximation / Method > another name for the Stationary Phase Approximation.
Sagnac Effect > s.a. atomic
physics; kinematics
of special relativity; tests
of newtonian gravity.
* Idea: The fact that,
if we send two light rays in opposite directions around a rotating
ring (say, on the surface of the Earth), they return with a time difference
proportional to
and
the enclosed area, and the interference depends on
.
* Applications: Laser
gyroscope, used for inertial guidance, based
on beats between the two rays.
@ Early work: Michelson PM(04); Sagnac CR(13); Michelson et al
ApJ(25) [experiment].
@ General references: Logunov & Chugreev SPU(88);
Anderson et al AJP(94);
Rizzi & Tartaglia gq/98;
Klauber FPL(03)gq/02 [general
case].
@ With matter waves: Gustavson et al PRL(97)
[atom interferometer and Earth's rotation]; Lenef et al PRL(97)
+ pn(97)feb;
Rizzi & Ruggiero
GRG(03)gq,
gq/03-in
[and Aharonov-Bohm effect], GRG(03)gq.
@ In general relativity, curved spacetime: Ashtekar & Magnon JMP(75);
Tartaglia PRD(98)gq;
Gogberashvili FPL(02)gq/01;
Sivasubramanian et al gq/03 [and
gravitational waves]; Camacho GRG(04)gq/03 [non-Newtonian];
Ruggiero GRG(05)
[and Aharonov-Bohm effect].
@ Related topics: Wucknitz gq/04/FP
[and closed Minkowski spacetime]; > s.a. Galilean
Group [boosts and Sagnac phase].
> Online resources:
MathPages page; Wikipedia page.
Saha Equation
*
Idea: Relates energies of states to temperature and number
densities; It allows us to infer densities of various ions from spectral line
intensities.
Salpeter Equation > see modified quantum mechanics.
Sampling > s.a. information.
@
Shannon sampling: Kempf PRL(00)ht/99 [generalization,
unsharp coordinates]; Smale & Zhou BAMS(04).
Sand Pile > see critical phenomena.
Sandwich Conjecture
* Idea: The conjecture
that, given two spatial metrics q and q' on two hypersurfaces
in spacetime, there is unique see that will interpolate between them,
up to gauge.
* Thin sandwich: The
hypersurfaces are infinitesimally close; One specifies the spatial field configurations
and their t-derivatives.
* Thick sandwich: The hypersurfaces are a finite distance apart.
@ General references: Bergmann in(70); Christodoulou & Francaviglia
in(79), RPMP(77);
Teitelboim in(82).
@ Thin sandwich: Bartnik & Fodor PRD(93)gq;
Giulini JMP(99)gq/98 [Einstein
+ gauge theory + scalar]; York PRL(99)gq/98 [and
initial-value
problem]; A Komar; Bartnik & Isenberg gq/04-in;
Pfeiffer & York PRL(05)gq [conformal,
uniqueness].
Satellites > see solar planets.
Scalar Fields > s.a. klein-gordon fields.
Scalar Product > see vectors.
Scalar Theory of Gravitation > s.a. matter
phenomenology; scalar-tensor.
* History: Started with Nordström's attempt at developing a special
relativistic theory of gravity.
@ Nordström's theory: Nordström AdP(13);
Einstein & Fokker AdP(14); in Pauli 58; Wellner & Sandri
AJP(64);
Harvey AJP(65);
Norton AHES(92)
[history]; Bauer mp/04 [self-gravitating
particles].
@ Equations of motion: Arminjon RJP(00)ap [with
preferred frame]; Kaniel & Itin gq/99;
Beig et al PRL(07)gq/06
[helically symmetric N-particle solutions].
@ PN approximation: Arminjon gq/01-in, gq/03-in.
@ As model: Watt & Misner gq/99 [for
numerical gravity]; Sundrum ht/03;
> s.a. modified general relativity [analog].
@ Related topics: Bezerra et al MPLA(02)
[2+1, including black hole]; Giulini SHPMP(08)gq/06 [history
and assessment].
Scalar-Tensor Theories of Gravity
Scalar-Vector Theories of Gravity > see theories of gravity.
Scalar-Vector-Tensor Theories of Gravity > see MOND; theories of gravity.
Scale Relativity
* Idea; A theory based
on the idea that physics must apply to coordinate systems in all "states
of scale"; Spacetime is described as a non-differentiable continuum, a
fractal which depends explicitly on internal scale variables.
@
General references: Nottale IJMPA(92);
Nottale 93; Nottale CSF(94)
[fractal spacetime]; Célérier & Nottale JPA(04)qp/06 [quantum
mechanics
and fields].
@ Applications to various theories:
Castro ht/96 [strings];
Nottale
et al JMP(06)ht [gauge
theory];
Célérier & Nottale JPA(06)qp [Pauli
equation]; Hammad JPA(08)
[derivation of Pauli and Dirac equations].
Scale Symmetry > see conformal symmetry.
Scaling > s.a. Critical
Phenomena [scale-free
networks]; entropy; fractal; phase
transition; renormalization group.
* Idea: The p-point correlation functions can be written in terms
of the 2-point correlation function or variance.
* Scale-free distribution:
One given by a power law, as opposed to an exponential with a scale in the
exponent; Power laws seem to be prevalent in nature, and may signal an underlying
universality.
* In galaxy distribution: Expected if an initially Gaussian distribution
of density fluctuations evolves under the action of gravitational instability.
@ General references: Wiesenfeld AJP(01)RL;
Henkel NPB(02)
[in statistical mechanics]; West CSF(04)
[renormalization group, complexity].
@ In biological systems:
Brown & West 00 [in biology]; West & Brown PT(04)sep.
@ In other areas: Peterson
AJP(02)phy/01 [Galileo
and the geography of Dante's Inferno]; > s.a. galaxy
distribution, turbulence.
Scarring > see quantum chaos.
Scharnhorst Effect > see casimir.
Schemes > s.a. Algebraic
Geometry.
*
Applications: Used in algebraic topology, number theory, ...
@ References: Eisenbud & Harris 92, 00.
Schläfli Formula
* Idea: A formula relating
the variations of the dihedral angles of a smooth family of polyhedra in a space
form to the variation of the enclosed volume.
@ References: Souam DG&A(04)
[for immersed piecewise smooth hypersurfaces in Einstein manifolds].
Schouten-Nijenhuis Bracket > see killing tensors [Killing-Yano].
Schreier's Conjecture
$ Def: The outer automorphism group of any finite simple group is solvable;
Has been proved.
Schrödinger Representation of Quantum Theory > see representations of quantum theory.
Schrödinger's Cat > see experiments in quantum mechanics; quantum states.
Schubert Cell > see grassmann.
Schubert Symbol
$ Def: Any non-decreasing
finite sequence of integers {pi}, i =
1,..., n,
i.e.pi in N,
with 1
p1
...
pn
m.
Schur's Lemma
$
Def: In a finite-dimensional irr of a group G, the
only elements which commute with all others are multiples of the identity.
Schwarz Inequality > see inequalities.
Schwarz Space > see distribution.
Schwarz Transformation > see analytic functions.
Schwarzschild Spacetime > s.a. coordinate expressions.
Schwarzschild-de Sitter Spacetime
Schwinger Effect > see particle effects.
Schwinger Function > see green functions in quantum field theory.
Schwinger-Dyson Equation > s.a.
[Wikipedia
page]; quantum gravity and renormalization.
@ References: Lyakhovich & Sharapov JHEP(06)
[for non-Lagrangian field theory].
Schwinger Model > see dirac fields; modified QED.
Scri ("Penrose script I") > see asymptotic flatness and null infinity.
Second Countable Topological Space > see types of topologies.
Second Fundamental Form > see extrinsic curvature.
Second Law of Thermodynamics > see thermodynamics.
Second Order Equations > see elementary algebra.
Second Quantization > s.a. quantum
field theory.
* Idea: It is a field
quantization, not really a second quantization.
* Motivation: Seems
necessary in order to obtain a consistent Lorentz-covariant quantum theory
of particles.
* Commutation relations:
The commutation relations between creation and annihilation operators corresponding
to a given set
of modes
in a classical field theory are related to properties of the classical modes
by [a(
), a
(
')]
= 
|
'
.
Sectional Curvature > see riemann tensor.
Seebeck Effect > see electricity [thermoelectricity].
Seesaw Mechanism > s.a. neutrinos; cosmological
constant.
* Idea: A mechanism by
which a phenomenon with very high characteristic energy scales can be seen at
much lower energies.
Segal-Bargmann Transform > see coherent states; Holomorphic Functions.
Segre Classification of Traceless Ricci Tensors
@ References: Zachary & Carminati GRG(04)
[algorithm].
Seiberg-Witten Map, Theory > s.a.
non-commutative gravity.
@ References: Marcolli dg/95-ln;
Flume et al NPB(97)
[Leff uniqueness],
ht/96 [rev];
Morgan 96; Adam et al JMP(00)
[solutions]; Ghosh JPA(03)
[map, interpretation].
Seifert Forms
Seifert Manifolds
* Idea: Quotient manifolds,
for example of the form S3/G, where G is a finite subgroup of SU(2); > s.a. Wikipedia.
@ References: Hikami CMP(06) [quantum invariants].
Seifert-Van Kampen Theorem > see fundamental group.
Selberg's Trace Formula > see Trace Formulas
Self-Adjoint Operator > see operators.
Self-Dual Fields > s.a. self-dual solutions in general relativity.
Self-Energy > see classical field theory; energy.
Self-Force > s.a. [semiclassical general relativity (back-reaction)], energy-momentum tensor [pN].
Self-Organization > s.a. critical phenomena.
@ References: Nicolis & Prigogine 77 [non-equilibrium systems]; Olemskoi
et al PhyA(04)
[with order-parameter field].
Self-Similarity
* For solutions
of Einstein's equation:
In the spherically symmetric case, a spacetime in which all dimensionless
variables depend only on z:= r/t.
@ General references: Embrechts & Maejima 02 [self-similar processes].
@ For spacetime metrics, kinematical: Coley CQG(97)gq/96;
Carr & Coley CQG(99)
[rev]; > s.a.
spherical symmetry.
@ For spacetime metrics, in general relativity: Carot & Sintes
in(97)gq/00 [fluid];
Harada CQG(01)
[pfluid, stability criterion]; Martín-García & Gundlach
PRD(03)gq [scalar];
Harada & Maeda CQG(04)
[scalar, stiff fluid, stability]; Maeda & Harada gq/04-in;
Carr & Coley GRG(05)gq [similarity
hypothesis]; > s.a. bianchi
IX; bianchi
models; critical collapse; spherical
symmetry.
Semialgebraic Geometry > see rings [partially ordered].
Semiclassical Field Theory > see QED; semiclassical general relativity; states in quantum field theory.
Semiclassical Quantum Mechanics
Semiconductors > see electricity.
Semicontinuity, Upper / Lower
$ Def: A function is
said to upper/lower semicontinuous at a point x if...
Semidirect Product of Groups
$ Def: Given a group G and
an Abelian group V, with a G-action
on V, their semidirect product G
s V is
the set G × V with
the composition law (g1, v1)
(g2, v2):=
(g1g2, v1+g1v2).
* Remark: We can thus
get a new group from every representation of G,
with
V
s G/V =
G.
@ References: Geroch & Newman JMP(71).
> Examples: see the poincaré group and
the BMS
Group.
Semigroup > s.a. poincaré group.
$ Def: A set with an associative composition law (an associative groupoid).
* Special types: Additive
or Abelian if commutative; Cancellative if a + c = b + c implies a = b; > s.a. Monoid;
Semiring.
* Topological semigroup: Theory created by A D Wallace.
* Applications: Irreversible
dynamics, both in classical mechanics (> see Transport)
and in quantum mechanics (& Prigogine, Bohm, > see dissipation,
modified quantum mechanics); Non-deterministic
dynamics (Blanchard & Jadczyk); > s.a. arrow
of time.
@ General references: Wallace BAMS(55);
Carruth, Hildebrant & Koch 83; Steinberg JCTA(06)
[representations, and Möbius functions].
@ Quantum dynamical semigroups: Davies JFA(79)
[generators]; Alicki qp/02-in;
Antoniou et al OSID(02)
[implementability];
Courbage IJTP(07)
[unstable states]; Harshman IJTP(07)
[from underlying Poincaré symmetry]; Bohm et al IJTP(07) [from causal
symmetries]; > s.a. neutrons [interferometry].
Seminorm > see norm.
Semiorder > see posets [generalizations].
Semiring > s.a. Burnside Ring.
$ Def: A semigroup
with distributive multiplication.
* Of subsets of a set:
A collection R of subsets of a set X such that Ø, X in R,
and R is closed under intersection.
Semisimple Group > s.a. lie
groups and representations.
$ Def: One with no (proper, non-trivial)
invariant Abelian subgroup.
* And other structure:
A n.s.c. for them to have a non-degenerate metric is that kab:= Camn Cbnm be
non-singular.
* Semisimple Lie groups:
They are locally isomorphic to products of simple groups; These groups have
a very rich structure and have been completely
classified
early.
Separable Hilbert Space > see hilbert space.
Separable Topological Space > see types of topologies.
Separation of Variables > see hamilton-jacobi; schrödinger equation.
Separatrix
* Separatrix mapping:
The mapping that gives the energy and phase of a perturbed non-linear pendulum
near the
separatrix after a velocity pulse (swing), in terms of their values before;
It shows that the reason for the emergence of local instability is the sensitivity
of the variation in phase on the orbit.
@ References: in Zaslavskii et al 91, p39; Wiesenfeld JPA(04)
[Hamiltonians with symmetries, existence].
Sequence Transformation
@ References: Wimp 81.
Sequential Dynamical Systems
* Idea: a class of discrete
dynamical systems which significantly generalize many aspects of systems such
as cellular automata, and provide a framework for studying
dynamical processes over graphs.
@ References: Mortveit & Reidys
07.
Series > s.a. summations.
Serret-Frenet Equations > see minkowski space.
Sesquilinear Form > see Quadratic Form.
Sextic Equation > see elementary algebra.
Shannon Coding, Information, Sampling > see information; Sampling.
Shear of a Congruence of World-Lines
$ Def:
If ua is the unit timelike
tangent vector to the congruence, one defines the traceless shear tensor and
the shear scalar as
ab:=
ab –
qab ,
:=
(
ab
ab)1/2 .
where
ab is the expansion tensor and
the expansion
scalar of the congruence, and qab the
spatial metric qab = gab +
ua ub.
Shell, Gravitating > see gravitating matter; metric matching; models in canonical gravity; semiclassical general relativity; spherical symmetry.
Shift Vector > see initial value formulation of general relativity.
Shimura-Taniyama-Weil Conjecture > see number theory.
Shock Waves > see Gastrophysics; foliations, numerical general relativity [gauge shocks]; gravitational radiation; phenomenology of higher-order gravity; velocity.
Short Exact Sequence > see exact sequence.
Shot Noise > see Noise.
Sigma-Algebra (
-Algebra)
$ Def: A collection
of subsets of a set X with
three properties: (a) The empty set is in the collection; (b) The complement X\A of
any set A in
is
also in
; (c) The union
of countably many sets in
is
also in
.
* Relationships: A
-algebra
is a
-ring with the added
requirement of property (a).
* Generating a sigma algebra:
Given any collection
of
subsets of X, there
exists a unique
-algebra
generated by it, defined as the intersection of all
-algebras
that contain
(this set is not empty,
since the power
set
of X is in it, for example); It is easy
to
verify
that
this
object
is in fact a
-algebra, and
it is also clearly minimal.
Sigma-Field (
-Field) > see ring.
Sigma Ring (
-Ring) > see ring.
Signature of a Metric > see metric; modifications of general relativity [signature change]; spacetime models and dynamical metric models.
Silent Universe
@ References: Bruni et al ApJ(95)ap/94, gq/96-in
[Bianchi I with B field, singularities], Mars CQG(99)gq [3+1
description]; Van den Bergh & Wylleman CQG(04)gq [Petrov
I with cosmological constant].
Silver Mean
* Value: The
number
+
1 = 2 + 1/(2 +
1/(2 + ...)).
Simon-Mars Tensor
* Idea: A tensor on
the manifold of trajectories in spacetime.
@ References: Bini et al CQG(01)gq [congruence
approach]; Bini & Jantzen NCB(04)gq-in
[stationary spacetimes].
Simple Group > see group types.
Simplicial Complex > see cell complex.
Simply and Multiply Connected Spaces > see connectedness.
Simply Transitive Action > see group action.
Simultaneity > s.a. kinematics
of special relativity; hidden
variables; types of gauge theories [fiber
bundle formulation].
@ References: Jammer 06 [history; r PT(07)aug, JPA(07)#40].
Sinai's Theorem
* Idea: A box of hard
spheres is a chaotic system.
@ References: Sinai UMN(70).
Sine-Gordon Equation > s.a. partial
differential equations.
* Idea: An equation
for a (1+1)-dimensional field with solitonic solutions.
@ General references: Schief PRS(97)
[2+1, integrable]; Dorey & Miramontes NPB(04)
[homogeneous,
mass scales and crossover].
@ Solitons: Gegenberg & Kunstatter PLB(97)ht, ht/97-in
[and dilaton gravity]; Christov & Christov PLA(08)
[description as point particles,
and quantization].
Singletons
* Idea: Unitary non-decomposable
reps of the (3+2) de Sitter group; They have strange gauge transformation
properties and can be gauged away to zero on any compact set, so they really
live at infinity; Spin 0 or 1/2.
* Uses: Fronsdal
has proposed that leptons are made of a Fermi singleton ("Di")
and a Bose one ("Rac").
@ References: Flato & Frønsdal CMP(87),
JGP(88); Flato et al ht/99-in
[rev]; Frønsdal
LMP(00)ht/99 [and
neutrinos].
Singular Values
* Idea: A Generalization
of the concept of eigenvalues.
Singularities for Differential Equations > see partial differential equations; wave phenomena.
Singularities for Mappings > s.a. Catastrophe; Cusp;
Fold.
@ General references: Whitney AM(55); Arnold
91.
@ Surface singularities: Kiyek & Vicente 04 [resolution, in characteristic zero].
Singularities in Spacetime > see censorship; types of singularities.
Sinh-Gordon Equation
@ References: Xie
& Tang NCB(06) [solution method].
6j-Symbols > see SU(2).
Skein Relations > see knot theory and physics.
Skein Space > see spin structures.
Skeleton of a Simplicial Complex
$ Def: Given a simplicial
complex K in Rn,
its p-skeleton K(p)
is the set of all
in K of dimension
p.
* Example: The elements
of K(0) are the vertices of K.
Sky > see geodesics.
Skyrmion Model > s.a. [QCD
phenomenology]; astronomical objects [skyrmion stars].
* Idea: A phenomenological
model for QCD that contains the
fields
as basic fields, and constructs the nucleons as solitonic solutions in the
pion fields, corresponding to bound states of pions; A "Skyrme term" has
to be present in the Lagrangian for stability, and the collective coordinate
method is used for quantization; > s.a. black hole
solutions, black hole
hair.
@ General references: Gisiger & Paranjape PRP(98);
Cho et al ht/99;
Abbas PLB(01)
[and hadrons];
Wong hp/02, hp/02, hp/02;
Cho et al IJMPA(08)ht/04 [interpretation];
Rajeev a0801 [relativistic
wave equation].
@ Quantization:
Jurciukonis et al JMP(05)nt [SU(3)
model, canonical quantization]; Krusch ht/06 [overview].
@ Skyrme black holes: Zaslavskii PLA(92)
[first law of thermodynamics]; Shiiki & Sawado CQG(05)gq [
< 0];
Brihaye & Delsate MPLA(06)ht/05 [in
de Sitter];
Nielsen PRD(06)gq [isolated
horizons];
> s.a. black hole hair.
@ And gravity:
Ioannidou et al PLB(06)gq [gravitating],
PLB(06)gq [spinning];
> s.a. topology change.
Slice
$ Def: A closed achronal
subset of spacetime without edge.
Slingshot Effect > see orbits in newtonian gravity.
Smale Conjecture > see diffeomorphisms.
Smarr Formula
* Idea: A formula that
gives the mass of a stationary black hole in terms of quantities defined on
its horizon, such
as area and surface gravity; For Kerr-Newman black holes,
M = (
/4
)
A +
· J +
Q .
* Remark: It looks
like the "integrated version" of the first law,
but the latter holds for any perturbation, not just stationary ones.
@ References: Smarr PRL(73)
[Kerr]; Breton GRG(05)gq/04-in
[in non-linear electromagnetism]; Barnich & Compere PRD(05)gq/04 [higher-dimensional
Kerr-AdS].
Smith Conjecture / Theorem > see spheres.
Smooth Particle Hydrodynamics > see fluid.
Smoothing > see Coarse-Graining; relativistic cosmology.
Snell's Law > s.a. Refraction.
@ References: Heller AJP(48)
[teaching]; Drosdoff & Widom AJP(05)
[photon beam point of view].
Sobolev Space
$ Def: The Sobolev
space Wpm(U)
is the space of all functions which belong,
together with their
derivatives up
to the m-th order, to Lp(U):
Wpm(U):=
{f | Dj f
Lp(U)
for all j such that | j |
m}
.
* Special case: For p = 2, we call Hm(U):=
W2m(U).
@ References: Adams 75.
Soldering Form > s.a. spin
structure.
* Idea: A "disguised
identity", also called Infeld-Van der
Waerden Symbol, that establishes an isomorphism between spin tensors and spacetime
tensors.
* SL(2, C)
spinors:
The objects that correspond to spacetime vectors are the self-conjugate spinorial
2-tensors, and the soldering form takes
Va → VAA', with Va
=
aAA' VAA', or VAA' =
aAA' Va ;
With the right choice of basis, these
's
can be thought of as the unit 2 × 2
matrix and the Pauli matrices.
* SU(2) spinors: Objects
corresponding to spacetime vectors are symmetric spinorial 2-tensors, and
the soldering form takes
Va → VAB, with Va
=
aAB VAB, or VAB
=
aAB Va ;
With the right choice of basis, these
's can be thought of as the
three Pauli matrices.
* 4-spinors: The soldering
form corresponds to the Dirac matrices.
* Applications: The
(complexified) SU(2) soldering form has been used as
a variable for gravity.
Solenoidal Vector Field > see vector field.
Solid State Physics > see condensed matter.
Solutions of Einstein's Equation
Solvability, Solvable Equation > s.a. classical
systems; wave equation [exactly
solvable].
@ References: Pesic 03 [Abel and
the quintic].
Solvable Group
$ Def: G is
solvable if it has a normal series whose factors are Abelian (solvable series);
Or,
if the chain G = Q0
Q1
Q2
...,
where Qi
is the commutant of Qi–1,
has Qm = {e}
for some m (the height of G).
* Properties: A solvable
group always has a commutative invariant subgroup (the Qm–1 above).
* Examples:
- The 2D Euclidean group, of
height 2, E2 = T1,1 ×s SO(2)
T2
{e}.
- The 2D Poincaré group: P2
= T1,1 ×s SO(1,1)
T1,1
{e}.
- The Heisenberg group.
Space in Mathematics
$ Def: (Souriau) A set E is
a space if there is a recueil R (of "glissements") acting
on E.
* And other structure:
A space has a natural topology, in which F
E is
open
if idF in R.
Space in Physics > s.a. spacetime
models [absolute space]; tensor decomposition [for spacetime metric].
* Idea: Given a spacetime
manifold (M, g) and a time function f on M,
space
is a level set for f.
@ References: Lachièze-Rey A&A(01) [for an arbitrary observer].
Spacetime > s.a. decomposition; important subsets; models in general and discrete models; topology; types.
Spacetime Algebra > see Geometric Algebra.
Sparking of the Vacuum > see vacuum [QED effect].
Sparling Forms > s.a. stress-energy
pseudotensors.
* Real 2-forms: The set
of four 2-forms given by
I := –
IJKL
JK
eL
,
where eL is a tetrad field, and
JKa = eJb
a ebK its
Levi-Civita connection.
* Complex 2-forms: The two sets of forms
(+/–)I :=
–
IJKL
(+/–) JK
eL
,
where
(+/–) JK:=
(
JK
i
JKLM
LM).
* 3-form: A tetrad-dependent
3-form
I or
(+/–)I on
the bundle of orthonormal frames over spacetime, which is a potential for a
local energy-momentum density
I
for the gravitational field; If e*J is
a basis of 3-forms, and GIJ the
Einstein tensor,
d
I =
d
(+/–)I =
I
+ GIJ e*J .
@ References: Dubois-Violette & Madore CMP(87); Goldberg PRD(88); Frauendiener CQG(89), GRG(90).
Special Functions > s.a. Integral
Transforms; representations of lie groups.
* Idea: Usually, complete
orthonormal sets of functions on some set X (typically,
an interval X = [a, b]), with which we approximate
a function by a finite sum f(x)
n=1N anUn(x),
where the coefficients are calculated by an =
X dx Un*(x) f(x)
and the finite sum minimizes
X dx |f(x) –
n anUn|2.
* Group theoretic approach: Most special functions are connected with
the representation of Lie groups; The action of elements D of the
associated Lie algebras as linear differential operators gives relations among
the functions
in a class – for example, their differential recurrence relations; & Gelfand, Naimark, N Ya Vilenkin.
* Bochner's problem: The characterization of classical orthogonal polynomial
systems as solutions of second-order eigenvalue equations.
@ General references: Rainville 63; Etingof & Kirillov Jr ht/93 [and
representation theory]; Temme 96 [intro]; Lorente JCAM(03)mp/04 [rev
of applications]; Batterman BJPS(07)
[what makes them special].
@ Related topics: Lucquiaud JMP(90)
[in curved space]; Peherstorfer mp/02 [zeros];
Gurappa
et al mp/02 [new
approach]; Eynard mp/05-in
[asymptotics];
Giraud JPA(05)mp [vanishing
average]; Simon BAMS(05)
[on S1]; Alhaidari AML(07)mp/05 [integrals];
Coftas CEJP(04)mp/06 [from
hypergeometric equations]; Bruschi et al JPA(07)
[from Diophantine conjectures]; Gómez-Ullate et al a0805 [generalized Bochner
problem].
@ Specific functions:
Raposo et al CEJP(07)a0706 [Romanovski
polynomials]; > s.a. Airy; bessel; Elliptic; Gamma; Hypergeometric;
Jost; Mathieu; Struve;
Whittaker; Zeta
Function; spherical
harmonics; other functions.
> Other polynomials:
see Chebyshev, Gegenbauer, Hermite,
integral equations, Jack, Laguerre and legendre
polynomials; graph and knot
invariants.
Special Relativity > s.a. doubly special relativity; kinematics.
Spectral Action > see non-commutative physics.
Spectral Decomposition > see hilbert space.
Spectral Function
@ References: Kirsten ht/00-wd
[review].
Spectral Sequence
@ References: in Spanier 66.
Spectral Theory > see operator.
Spectrometer > see experiments in physics.
Spectrum of an Algebra
$ Def: The set of its characters.
Spectrum of an Algebra Element
$ Def: The spectrum
of an element a of an algebra A over K is the set
of
K such
that a–
I
is not invertible,
(a):=
{
(a) |
a
character of a} .
Spectrum of an Operator > see operator theory.
Speed > see velocity; constants [speed of light]; tests of general relativity [speed of gravity].
Sphaleron > see solutions of gauge theories.
Sphere (including Sphere Packings).
Spherical Symmetry > s.a. spherical symmetry in general relativity; gauge theory solutions.
Spi > see asymptotic flatness.
Spin Echo Experiment
@ References: Ainsworth FPL(05)
[and approaches to statistical mechanics].
Spin Networks > s.a. connection representation of quantum gravity, and other spin models.
Spin-Statistics Theorem > s.a. particle statistics.
Spinors > s.a. 2-spinors; 4-spinors; in field theory.
Spintessence > see quintessence.
Spiral, Logarithmic {# s.a. Bernoulli.}
* Examples in nature:
Galaxies, Nautilus.
@ References: in Thompson; in Maor ThSc(94)jul.
Spline
@ References: de Boor 78.
Splitting of Spacetime > see decomposition.
Splitting Sequence > see exact sequence.
Splitting Theorem
@ Lorentzian geometry: Yau 82;
Galloway CMP(84),
JDG(89); Ehrlich & Galloway
CQG(90); Newman JDG(90); Galloway AHP(00)m.DG/99,
gq/02-in
[null].
Spontaneous Emission
@ General references: Crisp & Jaynes PR(69),
Leiter PRA(70)
[in semiclassical radiation theory]; Cray
et
al AJP(82)
[ito interference]; Milonni AJP(84)
[and fluctuation dissipation]; Olsen
et
al qp/05 [2-level
bosonic atom, phase space approach]; Kleppner PT(05)feb
[and stimulated, Einstein's 1917 paper].
@ Based on electron self-energy, without field quantization: Barut & Van
Huele PRA(85),
& Dowling PRA(87), & Salamin PRA(88).
Sprinkling of Points in a Manifold > see statistical geometry.
Square (magic square, ...) > see number theory.
Square Roots > see elementary algebra.
Squeezed States > s.a. distance; QED;
symplectic structure [squeezing].
* Idea: A quantum minimum-uncertainty
(
x
p =
/2)
state of an oscillator/field in which the complementary operators do not have
the
same variance; The product of the variances of course satisfies the uncertainty
relation, but one of them is lower than the coherent state value, the one
predicted by semiclassical models.
* Examples: Squeezed light may be applied in data transmission and
high-precision metrology.
@ General references: Yuen PRA(76);
Yuen & Shapiro OL(79);
Caves PRD(81);
Henry & Glotzer
AJP(88); Muñoz-Tapia AJP(93)
[properties]; Nieto qp/97-in
[history]; Beckers et al PLA(98)
[new sets]; Trifonov PS(98)
[for n observables]; Saxena
JPA(02)
[eigenvalue equation]; Honegger & Rieckers PhyA(04)
[non-classicality and coherence]; Sträng JPA(08)-a0708 [semiclassical
evolution].
@ On S1: Kowalski & Rembielinski
JPA(02)qp, JPA(03)qp;
Trifonov JPA(03)qp/02.
@ For QED, light: Loudon & Knight JMO(87)
[light]; Slusher & Yurke SA(88)may [light]; Putz & Svozil NCB(04)ht/01 [vacuum, e mass
shift];
Popp
et
al PLA(02)
[in biological systems]; Petersen et al PRA(05)qp;
Bachor et al CP(05);
Biswas & Agarwal PRA(07)
[photon-subtracted, non-classicality].
@ Other systems: Burgess PRD(97)
[non-equilibrium quantum field theory]; Tavassoly JPA(06)
[solvable]; Marchiolli et al PRA(07)qp [discrete].
@ Squeezed number states: Nieto PLA(97)qp/96;
Albano et al JOB(02)qp/01.
@ Generalized: Marchiolli & Galetti a0709; Shchukin
et al a0712.
> Relalated states and generalizations:
see coherent
states; fock space; Kerr
State; vacuum.
Stability > for matter, see condensed
matter; for solutions of dynamics, see classical
systems; for theories,
see physical
theories.
> In gravitation:
see black hole perturbations; cosmological
perturbations; perturbations
in general relativity.
Stability Theory in Mathematics > s.a. Bifurcation
Theory.
@ References: Yoshizawa 75; Rouche et al 77.
Stabilizer of a Group Element > see group action.
Stacks > see categories.
Standard Map > s.a. chaotic
systems.
* Idea: A chaotic, area
preserving discrete map of the unit square map onto itself used to model a kicked
rotator; Also called Taylor-Greene-Chirikov map;
Defined
by
pn+1 = pn + K sin(
n)
,
n+1=
n + pn+1.
@ References: Shevchenko PhyA(07).
> Online resources:
MathWorld page;
Wikipedia page.
Standard Model > see in cosmology and particle physics.
Star-Algebra > see abstract algebra.
Star-Convex Subset of an Affine Space > see affine structures.
Star Product > s.a. non-commutative
field theory; non-commutative geometry;
types of quantum field theories.
* Idea: An antisymmetric
tensor
mn used
to define non-commutative geometrical structures, such that for two functions f and g,
(f *g)(x):=
exp(
i
mn {
/
ym}
{
/
zn}) f(y) g(z)|y=z=x = f(x) g(x)
+
i
mn
m f(x)
n g(x)
+ h.o.t.
* Remark: This structure
is not Lorentz-invariant.
@ References: Zachos JMP(00)ht/99 [evaluation];
Gammella LMP(00)
[tangential]; Freidel & Krasnov JMP(02)
[and spin networks]; Man'ko et al PLA(05)ht/04 [dualities];
Pinzul & Stern NPB(08)
[gauging]; Kupriyanov & Vassilevich a0806 [friendlier approach].
Stark Effect > see atomic physics.
Stars > s.a. star types.
State of a System > s.a. quantum state.
State Sum Models > see spin foam.
Static Spacetime > see general relativity solutions with symmetries.
Stationary Phase Approximation >
s.a. Steepest Descent Approximation.
* Idea: An approximation
used to calculate the leading order behavior of integrals of the type
–inftyinfty dx f(x)
exp{i
(x)/
}
in the limit of small
;
Consists in taking into account only the contribution from the critical points
of
(x);
Related to the steepest descent approximation.
* In path integrals: The approximation of writing the field
as the classical solution plus a small perturbation; Sometimes known as
WKB or one-loop approximation.
@ References: Kamvissis mp/07 [and steepest descent].
Stationary Spacetime > see general relativity solutions with symmetries; types of spacetimes.
Statistics > s.a. error analysis in physics; particle statistics; probability.
Statistical Mechanics > s.a. non-equilibrium.
Steady State > see states of a system.
Steady State Cosmology > s.a.
cosmological models and general
relativistic models.
* History: First proposed
in 1948 by H Bondi, then T Gold and F Hoyle (and Littleton?); Despite its
loss of mainstream favor, to some extent the idea has been incorporated into
some versions of inflation.
* Idea: It postulates that
the universe is always expanding, and matter is created at precisely the rate
required to maintain a constant spatial density; A steady-state universe has
no beginning or end, and its
overall
properties are constant in time.
* And observation: They
don't have the singularity and flatness problems of the standard model, but they
were ruled out by observations on radio souces by M Ryle et al at Cambridge in
the 1950's and early 1960's, and especially by the discovery of the microwave
background.
@ General references: Hoyle in(58); Arp et al Nat(90)aug;
Andrews ap/01.
@ Quasi-steady state: Hoyle et al PRS(95)
[comment Wright MNRAS(95)], 00; Burbidge et al PT(99)apr
[and reply by Albrecht PT(99)apr];
Burbidge ap/01-in;
Narlikar
et al PASP(02)ap [acceleration], ApJ(03)ap/02 [and
cmb]; Vishwakarma & Narlikar JAA(07)-a0705 [and
repulsive gravity]; Narlikar et al JAA(07)-a0801 [and
cyclic universe].
@ Criticism of Big Bang: Arp & Van Flandern PLA(92);
Arp ap/98-in;
Lopez-Corredoira ap/03-in.
Steady State Equation > see partial differential equations.
Steepest Descent Approximation > see integration.
Stefan-Boltzmann Law > see thermal radiation.
Stein Structure > see 4D manifolds.
Stem > see posets.
Stephani Universe / Model
* Idea: A spherically
symmetric, inhomogeneous cosmological model, recently used as a possible explanation
of the cosmic acceleration.
@ General references: Stelmach & Jakacka CQG(06)
[angular sizes]; Pedram JCAP-a0806 [+ scalar, classical and quantum].
@ And acceleration: Stelmach & Jakacka CQG(01)-a0802;
Godlowski
et
al CQG(04)ap.
Stern-Gerlach Experiment > see experiments in quantum mechanics.
Stiefel Manifold of k-Frames > see differentiable manifolds.
Stiefel-Whitney Classes / Numbers
Stieltjes Constants
* Idea: The expansion
coefficients in the Laurent series for the Hurwitz zeta function about s =
1.
@ References: Coffey JMAA(06)mp/05
[evaluation], PRS(06)
[summation relations], a0706 [
j coefficients,
Hurwitz zeta function], a0706 [series
representations]; > s.a. MathWorld page.
Stieltjes Integral > see integration.
Stieltjes Transform
@ References: Schwarz JMP(05)mp/04 [generalized];
> s.a. MathWorld page.
Stimulated Emission > see quantum field theory in curved backgrounds [black holes]; Spontaneous Emission.
Stirling Formula
* Idea:
For n →
, n!
(n/e)n (2
n)1/2,
or ln n!
(n+
)
ln n – n +
ln(2
).
Stirling Numbers
@ References: Branson DM(06) [representation ito recurrence relations].
Stochastic Electrodynamics > see modified electromagnetism.
Stochastic Gravity > s.a. Induced
Gravity.
* Idea:
Based on the Einstein-Langevin equation, which has in addition sources due
to the noise kernel, the expectation value of the stress-energy bi-tensor
which describes the quantum matter fluctuations.
@ References: Ross & Moreau GRG(95);
Moffat PRD(97)gq/96;
Zakir ht/98-in;
Hu IJTP(99)gq;
Cole et al PRA(01)
[as residual van der Waals force]; Hu & Verdaguer gq/01-ln, CQG(03)gq/02, LRR(04)gq/03 + LRR(08)-a0802,
et al gq/03;
Verdaguer gq/06-in
[and applications].
Stochastic Layer / Region in Phase Space > see phase space.
Stokes' Law
* Idea: The friction
force on a small sphere of radius r moving with terminal speed v in
a homogeneous fluid of
viscosity coefficient
is
F = 6
r
v.
Stokes Parameters > see polarization.
Stokes' Theorem > see integration on manifolds.
Stone Space > see types of topologies.
Stone's Theorem
* Idea: It says or
implies that exp( i tH/
)
is unitary if H is self-adjoint,
even if densely defined unbounded, on an infinite-dimensional space.
Stone-von Neumann Theorem > see representations of quantum mechanics.
Strain Tensor
@ References: de Prunelé AJP(07) [in spherical coordinates].
Strange Star > see star types.
Strangelet / Strange Quark Nugget > see astronomical objects; experimental particle physics; QCD phenomenology.
Stratified Manifold > see types of manifolds.
Stratum (Plural: Strata)
* Idea: The set of all
orbits of the same topological type for the action of a group on a manifold.
@ References: Sartori & Valente JPA(03)
[compact linear G on Rn].
Stress > s.a. Elasticity; stress-energy
pseudo-tensors.
@ In mechanics and relativistic field theory: Gronwald & Hehl gq/97-in;
Medina AJP(06)
[contribution to energy and momentum].
Stress-Energy Tensors > see energy-momentum.
String Field Theory
@ Reviews: Kaku IJMPA(87);
Berkovits ht/01
[open superstrings]; Siegel 88-ht/01;
Thorn PRP(89);
Rastelli ht/05-in;
Taylor ht/06-in.
@ General references: Green & Schwarz PLB(84);
Hata et al PRD(86)
[covariant]; Witten NPB(86)
[and non-commutative geometry], NPB(96)
[open], pr(87); Horowitz et al PRL(86)
[cubic action]; Bowick & Rajeev
PRL(87),
NPB(87);
Strominger PRL(87);
Horowitz & Witt
PLB(87);
Bordes & Lizzi IJMPA(90);
Hashimoto & Itzhaki JHEP(02)
[observables]; Kling et al PLB(03)ht/02 [non-perturbative
solutions]; Bars ht/02 [Moyal
star formulation]; Drukker JHEP(03)ht [actions];
Okawa & Zwiebach JHEP(04)
[heterotic]; Taylor ht/04-ln
[perturbative computations].
String Theory > s.a. phenomenology; or under cosmic strings.
Strong Coupling Limit > see modified versions of general relativity.
Strong Interactions > see particle physics; QCD.
Strong Rigidity Theorem > see Rigidity.
Strongly Asymptotically Predictable Spacetime > see types of spacetimes.
Structural Realism, Structuralism
@ References: van Fraassen BJPS(06).
Structure Equations > see affine connection.
Structure Formation in Cosmology > see early universe.
Structure of Matter > see matter.
Structure of Physical Theories > see physical theories.
Structure Sheaf > see sheaf.
Struve Function
* Idea: The function
Hn(z) which satisfies the inhomogeneous Bessel equation z2 Hn''(z)
+ z Hn'(z) + (z – n) Hn =
(2/
) z/(2n–1)!!
Stückelberg Mechanism / Model > s.a.
classical particles [and Lorentz force]; particle
physics [standard model extension].
* Idea: A mechanism,
proposed in 1938 by Stückelberg, for making
an abelian gauge theory
massive while preserving
gauge invariance, by introducing an additional scalar field; 2004, Numerous
generalizations have been proposed for the non-abelian case, but the Higgs
mechanism in spontaneous
symmetry breaking remains the only known way to give masses to non-abelian
vector fields in a renormalizable and unitary theory.
@ General references: Dragon et al NPPS(97)ht
[variation – BRS-invariant polynomial form]; Ruegg & Ruíz-Altaba IJMPA(04);
Cianfrani & Lecian a0803-in-MPLA
[historical].
@ Quantization: Horwitz ht/98;
Oron & Horwitz FP(03)gq;
McKeon & Marshall ht/06 [renormalization and gauge invariance].
Sturm-Liouville Theory > s.a.
[ordinary differential equations]; matrices [determinants].
* History: Started
in the 1830's with Sturm and Liouville's generalization of the Fourier sine
series to expansions in terms of eigenfunctions of some ordinary differential
equations; The hardest
questions were those of convergence, resolved after 1900.
Subbase for a Topology
$ Def: A set of subsets
of X from which all open sets can obtained as arbitrary unions of
finite intersections.
Subgroup > see group theory.
Sublimation > see phase transition.
Submanifold > s.a. embedding; extrinsic curvature [including extremal surface]; Hypersurface; manifolds; spacetime subsets.
Submarine Paradox > see special relativity.
Submersion
$ Def: A smooth mapping f : M → B which
is onto, with f* onto for all p in M.
Subnormal Matrix / Operator
$ Def: (Halmos) A
non-square matrix A is subnormal if it can be completed to a (square)
normal matrix.
* Topology: The set
of such A's is not closed (can give example of A(t)
subnormal for all t > 0 but not for t = 0).
* Problem: Is there
an intrinsic characterization of such matrices?
Subobject of an Object A
$ Def: An object A'
in the same category, with a monomorphism f : A' → A.
Subspace of a Vector Space
* Idea: A subset which
is closed under the vector space operations; It can be characterized by a
multivector.
Substance > see Ontology.
Substantialism > see spacetime.
Subsystem > see quantum field theory formalism; quantum systems.
Sullivan-Baas Singularities > see riemannian geometry.
Sum Rules > see lattice gauge theories; standard model of particle physics.
Summations > s.a. series.
Sunyaev-Zeldovich Effect > see cosmic microwave background.
Superalgebras > see poincaré algebra.
Superbradyons > see causality violations.
Superconductivity > s.a. types of superconductors.
Superenergy Tensor > see stress-energy pseudotensors.
Superfields > see BRST; supersymmetric field theory.
Superfluids > s.a. Bose-Einstein
Condensation;
particle statistics; Quasiparticles; sound;
turbulence.
* Examples: In 4He,
pairs of atoms condense into a macroscopically coherent quantum state (Bose
condensation), which manifests itself as a frictionless
fluid; in 3He, the situation is not so simple;
He II (0 to 2.172 K) is a superfluid, highly heat-conductive by friction-free
convection;
He
I (2.172 to 4.2 K) is an ordinary fluid; 2005, Evidence seen in solid hydrogen
[@ news pn(05)mar].
* Method: Study using second-waves, regions with different concentrations
of ordinary/superfluid components.
* Properties: They exhibit
quantized vortices when rotated or subject to a T gradient.
@ General references: Feynman RMP(57);
Khalatnikov 65; SA(76)dec; Collins PT(92)jun;
news pn(96)oct;
Guénault 03; Adams & Bry PhyA(04);
Annett 04 [intro];
Brandão NJP(05)
[order parameter and entanglement]; Balibar CP(07);
Pilati et al PRL(08)
[critical T, 2D and 3D].
@ 3He: Bunkov et al PRL(00)
[sets of 4 atoms?]; Finne et al Nat(03)aug
+ pn(03)aug
[criterion for the onset of turbulence]; Volovik cm/07 [history].
@ In general relativity and cosmology: Carter gq/99-in
[vortex dynamics], G&C(00)ap [neutron
stars]; Casini & Montemayor
gq/99 [covariant];
Volovik PRP(01)gq/00 [analogs];
Garcia de Andrade gq/05 [with
torsion].
@ Examples: Donnelly pw(97)feb
[rotons]; Kapusta PRL(04)ht [for
Dirac neutrinos]; Bulgac et al PRL(06)
[spin-1/2 fermions].
@ History: Andronikashvili 90; Donnelly PT(95)jul;
Balibar phy/06 [discovery].
Superluminal Communication / Propagation > see causality violations; wave phenomena.
Supermanifold > see manifolds.
Supermetric > see geometrodynamics.
Supernova > see star types.
Superoscillations > s.a. schrödinger
equation; wave
phenomena.
* Idea: The phenomenon by which differentiable functions can locally oscillate on length
scales
that
are
much
smaller than the smallest wavelength contained in their Fourier spectrum.
Superparticle > see quantum particles.
Superposition Principle > related
to Linearity.
* In classical field theory:
Holds when the field equations are linear, so that a linear combination of
solutions is
a solution.
* In quantum mechanics: The space
of states of quantum theory is a vector space; Linear superpositions of states
are also allowed states.
@ In classical field theory: Notte-Cuello & Rodrigues mp/06 [and
energy-momentum conservation].
@ In quantum mechanics: Károlyházy in(90) [breakdown];
Greenberger et al PT(93)aug
[and interferometry]; Cirelli et al JGP(99)
[extension]; Bassi & Ghirardi
PLA(00)qp [against],
d'Espagnat PLA(01)qp [reply];
Peacock qp/02 [suggested
explanation]; Lan qp/03 [superposition
mixture];
Corichi GRG(06)qp/04 [and
geometrical formulation]; Lynn & Caponigro qp/06 [epistemological].
@ In quantum mechanics, systems / states: Morimae & Shimizu PRA(06)
[macroscopically distinct states]; Dowling et al PRA(06)
[atom and molecule].
Superpotential > see conservation laws.
Superradiant Scattering > s.a.
black hole analogs;
black hole radiation.
* Idea: The amplification
of a wave scattering off a black hole, a wave analog of the Penrose
process for energy extraction, which can be interpreted as stimulated
emission.
* Conditions: It
occurs only for bosonic fields.
@ References: Zeldovich JETP(72); Starobinskii JETP(73);
Bekenstein PRD(73);
Wald PRD(76); & Misner;
Bekenstein & Schiffer
PRD(98)gq;
Winstanley PRD(01)gq [scalar
in Kerr-Newman-AdS black holes].
Superscattering Matrix
Supersolids > see condensed matter.
Superspace > for space of geometries, see geometrodynamics; for bosonic + fermionic coordinates, see manifolds [supermanifolds].
Superstatistics > see statistics.
Supersymmetry > s.a. lie
algebras [superalgebras]; modified quantum mechanics.
* Supersymmetry group:
An extension of the Poincaré group of flat spacetime isometries to symmetry
transformations between integer and half-integer spin fields; Its generators Q change
the spin by 1/2, and the number N that classifies
susy theories
is like a "degree of kinship" between bosons and fermions.
* Supersymmetry algebra:
A graded Lie algebra, with generators {QiA, Q*j'B, Pa},
with i, j ' = 1, 2 (spinor indices), a, b =
1, ..., 4 (spacetime
indices), and A, B = 1, ..., N, with commutation relations
{QiA, Q*j'B}
= 2
ij'a Pa
AB
, {QiA, QjB}
= {Q*i'A, Q*j'B}
= 0 , [Pa, QiA]
= [Pa, Q*i'A]
= 0 , [Pa, Pb]
= 0 .
@ References: Cornwell 92; Jolie SA(02)jul; Ichinose ht/06,
ht/06 [graphical
representation].
> In field theory: see supersymmetry
in field theory; supersymmetry phenomenology; supersymmetric
theories.
Supertranslation > see asymptotic flatness.
Surface > s.a. Area;
dynamical triangulations [random]; Singularities.
* Flexible: A surface
in a smooth manifold M is called flexible if, for any diffeomorphism
on
the
surface, there is a diffeomorphism on M whose restriction
on the surface is
and which is isotopic to the identity.
@ In 3D euclidean space:
Guzzardi & Virga PRS(07)
[constant mean curvature].
@ In 4D manifolds: Hirose & Yasuhara Top(08) [flexible surfaces].
@ Deformations: Capovilla & Guven CQG(95).
Surface Gravity > s.a. laws
of black hole dynamics.
* In Newtonian gravity:
The quantity g = GM/r2,
for a spherical body of mass M and radius r.
$ For a black hole:
If l is the stationary Killing vector field of a black hole, normalized
at infinity, then
is
defined by l b
b l a =
l a;
It is constant over the horizon surface.
* Schwarzschild black hole:
Given by
= GM/(2G