Topics, L
L-Functions
@ References: Gelbart & Miller BAMS(04).
Lace Expansion > see ising model.
Ladder Operators > s.a. annihiliation and creation operators.
* Idea: A set of generalized
raising/creation and lowering/annihilation operators.
@ References: Ben Geloun & Klauder a0906 [for
continuous spectra, and coherent states].
Lagrange Bracket > see phase space.
Lagrange Spaces
* Idea: Spaces with non-linear
connections.
@ References: Miron & Anastasiei 93.
Lagrange Structure > s.a. path
integrals.
* Idea: A structure that
is more general than the Lagrangian formalism in the same sense as Poisson geometry
is more general than the symplectic one.
Lagrangian Formulation of a Theory > s.a. examples of lagrangian systems; higher-order lagrangians.
Lagrangian Observers > see Observers.
Lagrangian Submanifold > see symplectic structure.
Laguerre Polynomials > s.a. coherent
states [generalized Laguerre
functions].
* Generalized: Solutions
y = Ln(r)(x)
of the equation xy'' + (r + 1 – x) y' + ny = 0.
@ References: Moya-Cessa a0809 [new
expression].
Lamb Shift > see QED phenomenology.
Lambda Calculus
* Idea: May be regarded
both as a programming language and as a formal algebraic system for reasoning
about computation; Applied in the classical theory of computation, provides
a computational model equivalent to the Turing machine.
@ References: van Tonder SICOMP(04)qp/03 [for
quantum computation].
Lamé Equation, Functions, Operator
@ References: Ruijsenaars JMP(99), JMP(99)
[generalized]; Maier JDE(04)m.CA/02 [algebraic
solutions], PTRS(08)mp/03;
Takemura
m.CA/03, m.CA/04-in
[eigenvalues]; Bena et al PS(06)
[solitons, statistical mechanics].
Lanczos Lagrangian > see higher-order theories of gravity.
Landau Gauge > see gauge choices.
Landau Levels
@ References: Onofri IJTP(01)qp/00 [on
a torus].
Landau Model > see quantum particles.
Landau Pole Problem > s.a. QCD; QED; vacuum.
* Idea: The fact that,
in QED, the effective running coupling constant
has
a pole at a high, but finite value of the energy if renormalized.
* Status: In a non-Abelian
theory, solved by confinement and asymptotic freedom. <--??--> The problem
remains in the standard model of particle physics, because the coupling constants
for
the three interactions don't seem to join at the available energies, so we
don't see that the behavior is taken over by the non-Abelian nature of the
theory.
@ References: in Azam EJTP-a0806.
Landau-Ginzburg Model > see phase transitions; superconductivity.
Landau-Lifshitz Pseudotensor > see stress-energy pseudotensor.
Landauer's Erasure Principle > s.a. entropy;
information.
* Idea: The
loosely formulated notion that erasure of information produces heat, and at
least the equivalent amount of entropy; The erasure of n bits of
information must always incur a cost of k ln n in thermodynamic
entropy.
@ References: Plenio & Vitelli CP(01);
Bennett SHPMP(03);
Jacobs qp/05 [from
statistical mechanics]; Daffertshofer & Plastino PLA(05)
[derivation from entropy], PLA(07)
[in a gravitational field]; Maroney qp/07 [and
thermodynamics of indeterministic
operations]; Curilef et al PLA(08)
[extension to non-equilibrium systems].
Landé g-Factor > s.a. Gyromagnetic
Ratio.
@ References: Pfister & Pfister AJP(02)nov.
Landen Transformation > see Elliptic Functions [Jacobi].
Langevin Equation > see brownian motion; lattice field theory; quantum measurement.
Langlands Conjecture > see conjectures.
Langlands Program > see mathematics.
Laplace Transform > s.a.
bessel functions.
$ Def: Given a function
f, its Laplace transform is defined by Lf(k):=
dx f(x)
e–kx.
@ References: Corinthios PRS(07) [generalized].
> Online resources:
see MathWorld page.
Laplace Vector > see Runge-Lenz Vector.
Laplacian (Laplace-Beltrami) Operator > see laplace equation.
Lapse Function > see initial-value formulation of general relativity.
Large Deviations > see statistical mechanics.
Large Inductive Dimension > see dimension.
Large-N Expansion Method > see QCD.
Large-Number Hypothesis > s.a.
anthropic principle;
gravitational constant.
* Idea: In general, the
claim that, if two combinations of parameters of fundamental physical theories
and fundamental constants agree, it can't be a coincidence; Leads to predicting
relationships between parameters; In Dirac's words, "The Large Numbers
hypothesis asserts that all the large dimensionless numbers occurring in Nature
are connected
with the present epoch, expressed in atomic units, and thus vary with time.
It requires that the gravitational constant G shall vary, and also
that there shall be continuous creation of matter"; Related to what became
later known as the anthropic principle
* Examples: The main
ones involve the hierarchy problem for the fundamental interactions.
@ References: Dirac PRS(38),
PRS(74);
Carter pr(67)-a0710;
Dirac PRS(79)
[and modified general relativity]; Beesham IJTP(94), IJTP(94);
Mena & Carneiro PRD(02)gq/01 [and
holography]; Ray et al a0705/GRG
[rev]; Funkhouser PRS(08)phy/06 [and
cosmological constant scaling].
Larmor Formula > see radiation.
Larmor Frequency > see magnetism.
Laser > see optical technology; photons.
Laser-Ranging Experiments > see tests of general relativity.
LATOR Mission > see tests of general relativity with light.
Lattice Field Theory > s.a. lattice gauge theories.
Lax Tensor Equation / Pair > see integrable system.
Lebesgue Integral > see integration.
Lebesgue Number of a Cover > see cover.
Lee-Yang Circle Theorem > see functions [polynomials].
Lefshetz Fixed-Point Theorem > see fixed-point theorems.
Left Translation in a Lie Group
$ Def: The left action
of G on itself by L: G → G by Lg(h):=
gh.
Legendre Transformation > s.a. lagrangian
dynamics.
@ References: Zia et al AJP(09)jul [in classical mechanics, statistical mechanics
and thermodynamics].
Leibniz Principle
* Idea: The principle
of the identity of indiscernibles.
@ References: Castellani & Mittelstaedt FP(00)
[in classical and quantum physics].
Lemaître-Tolman-Bondi Solutions >
s.a. lensing.
* Idea: Spherically
symmetric dust solutions used to model matter collapse.
* And cosmological acceleration:
The solutions have also been used as models for an alternative explanation
of the dimming of distant supernovae based on the idea that
the acceleration
may be due to the effect of inhomogeneities on the global expansion;
According to this proposal we live in a special place in the universe, near
the center of a large spherical void
described
by a Lemaitre-Tolman-Bondi metric.
@ General references: Sussman & Trujillo CQG(02)gq/01 [dust];
Ribeiro CPC(02)gq [code
for null geodesics]; Sussman CQG(08)-a0709 [as
dynamical system]; Van Acoleyen JCAP(08)-a0808.
@ Cosmological acceleration:
Alnes et al JCAP(07)ap/05 [+
dust, do not account for acceleration]; Chuang et al CQG(08)ap/05;
Paranjape & Singh CQG(06)ap [and
averaging]; Garfinkle CQG(06)gq [dark-energy
model]; Romano PRD(07);
Enqvist GRG(08);
García-Bellido & Haugboelle JCAP(08)-a0802 [local
void]; Vanderveld et al a0904 [and
smoothness]; Célérier et al a0906 [giant
void not necessary].
@ Other phenomenology:
Garfinkle a0908 [motion of galaxy clusters].
@ Perturbations: Zibin PRD(08)
[scalar]; Waters & Nolan a0903 [self-similar,
gauge-invariant]; Clarkson et al JCAP(09)-a0903; > s.a. metric
matching.
@ Generalization:
Lasky & Lun PRD(06)gq [with
pressure].
@ Quantum: Kiefer et al PRD(07)gq [solution
of Wheeler-DeWitt equation, and Hawking radiation]; Bojowald et al PRD(08)-a0806,
PRD(09)-a0906 [in lqg];
Franzen et al a0908 [with
positive cosmological constant].
Length, Length Space > see distances; geometrical operators in quantum gravity; riemannian geometry [length scales].
Length Contraction > see kinematics of special relativity.
Length of a Map
@ References: in Gromov 81.
Lennard-Jones Fluid / Potential > s.a.
van der Waals Equation of State.
* Idea: A semi-empirical
potential used to represent the interaction between two molecules; It is strongly
repulsive for short separations, and weakly attractive for larger separations,
with an overall form u(r) = u0 [(r0/r)12 – 2(r0/r)6];
Can be used to obtain a van-der-Waals-type equation of state for a fluid.
@ References: Khordad PhyA(08)
[viscosity, integral equation method]; Romero-Bastida & Braun JPA(08)
[perturbations,
Lyapunov
modes]; Papari et al PhyA(09)
[thermal conductivity]; Celebonovic a0902-in [coexistence of phases, and application
to astronomy].
Lens Spaces > see 3D manifolds.
Lense-Thirring Effect > see tests of general relativity with orbits.
Lensing > see gravitational lensing.
Lenz's Law > see electromagnetic field equations; electricity.
Lepage Form > see hamiltonian dynamics.
Lepage-Dedecker Formalism > see symplectic structures.
Leptogenesis > see early-universe cosmology.
Leptons > see particle types.
Leptoquark > see GUTs.
Letelier-Gal'tsov Metric > see cosmic strings.
Levi-Civita Connection > see affine connection.
Levi-Civita Spacetime > s.a. types
of spacetimes.
@ General references: Magnon JMP(81)
[euclidean version from Wick rotation]; Konkowski et al CQG(04)gq, gq/04-in,
gq/04-in [quantum
singularities]; da Silva et al JMP(06).
@ Higher-dimensional: Sarioglu & Tekin PRD(09)-a0901;
Ponce
de León MPLA(09)-a0904.
Levi-Civita Tensor > see under Alternating Tensor.
Levinson's Theorem > see scattering.
Lewis Metric
* Idea: A stationary cylindrically symmetric vacuum solution of Einstein's equation.
@ References: Herrera & Santos JMP(98)gq/97 [geodesics];
Gariel et al JMP(00)
[mechanical interpretation of equations]; Davidson CQG(01)
[as exterior for rotating cylinder]; da Silva et al CQG(02)gq [rotating
shell source]; Ali NCB(04)
[rotating cylindrical sources]; Gariel et al JMP(06)
[and Painlevé transcendent
III].
Lewis Phase > see geometric phase.
Lewis-Papapetrou Metric > see types of spacetimes.
Lichnerowicz Conditions > see metric matching.
Lichnerowicz Equation
* Idea: An equation which
arises from the Hamiltonian constraint equation for the Einstein-scalar field
system in general relativity.
@ References: Hebey et al CMP(08)gq/07 [results
for compact manifolds].
Lichnerowicz Theorem > s.a. Hawking-Lichnerowicz
Theorem.
* Idea: A smooth, stationary,
topologically trivial and asymptotically flat vacuum solution of the Einstein
equation is just flat; Extends to electrovac Kaluza-Klein.
$ Def: If (M, g)
is topologically Euclidean, asymptotically flat and empty, and stationary,
with the electromagnetic and matter
current staticity conditions j[a kb]
= 0 and
u[a kb] =
0, where k is the stationary
Killing vector field, j is the
electric current vector and u the matter current vector appearing
in
Jmatterab =
ua
ub + pab,
then the staticity conditions F[ab kc]
= 0 and k[a;b kc] =
0 will also hold.
@ References: Lichnerowicz 55; Carter in(73).
Lichnerowicz-Obata Conjecture > see group action.
Lie Algebra [including generalizations]
Lie Group > s.a. examples and representations.
Lie-Poisson Manifold
@ Quantization: Racanière m.DG/04.
Liénard-Wiechert Potentials >
s.a. Robinson-Trautman Spacetimes [gravitational
analog].
$ Def: The electromagnetic
potentials for a charge moving with velocity u, normally written
in the form
![]()
where
s:= r – (r · u)/c,
and [ ] stands for "retarded".
@ References: Panofsky & Phillips 62; Jackson 75; Heras AJP(96)apr
[derivation]; Jackson IJMPA(02)hp;
Gsponer phy/06,
phy/06 [arbitrary
acceleration, complete current density].
Lifshitz-Type Theories > s.a. Horava
Gravity; renormalization.
* Idea: Field theories
with
different
scaling in the time and space directions.
Original theory (Lifshitz 41): A simple scalar theory, proposed in a study of
the behavior of critical points (such as the triple point) in condensed matter
systems,
with
the
usual
Galilean
invariance
of Newtonian mechanics but without
Lorentz
invariance,
in which Lorentz symmetry appears as
an accidental
symmetry
at
large
distances; Quantum corrections, which become larger at larger distances, give
rise to a Lorentz-invariant theory at distances much larger than the scale at
which the theory is defined.
@ References: Lifshitz ZETP(41).
Lifting of a Map
$ Def: Given two maps f : Y → X and p: E → X,
a lifting of f is a map g: Y → E,
such that pg = f.
Light Cone
@ References: in Klainerman & Nicolò book [properties of intersections];
Choquet-Bruhat et al CQG(09)-a0905 [light-cone
(cross-section area) theorem].
Limit Cycle
* Idea: A closed phase
curve, which represents oscillatory motion.
@ Method for finding: Delamotte PRL(93).
Lindblad Equation / Theory > s.a.
dissipation.
* Idea: A master equation
describing dissipative quantum dynamics / Theory of open/damped quantum systems.
@ Solutions: Nakazato et al PRA(06)qp [in
Kraus representation]; Brodier & Ozorio de Almeida a0808/PRA
[semiclassical, approximate].
> Generalizations: see Master Equation.
Lindelöf Property > see types of topologies.
Line, Line Bundle > see line.
Linear Space > see vector space.
Linearity in Physics > see electromagnetism; field theory; formulations of quantum mechanics; Non-Linear Quantum Mechanics; quantum field theory formalism and types; sigma models.
Link of a Vertex in a Simplicial Complex
$ Def: The union of
all subsets not containing v of the simplices that intersect v.
Link Theory > s.a. knots (+ invariants + in
physics); types of distances.
* Idea: May be algebraically described as certain morphisms in the
category of tangles.
* Linking number: Has
the properties lk(
1
2,
3)
= lk(
1,
3)
+ lk(
2,
3),
and lk(
–1,
) = –lk(
,
).
* Borromean rings: A set of three loops such that each pair is unlinked
but the three are linked together.
* Whitehead link: Has zero helicity.
@ Invariants:
Hillman 02; Jin & Zhang PhyA(04)
[Jones polynomials for some links]; Akhmetiev JGP(05)
[3-component links]; Chernov & Rudyak G&T(05)m.GT/03 [general
theory]; Buck & Flapan JPA(07)
[topological characterization].
@ In 4D: Bartel & Teichner G&T(99) [S2-links
are null-homotopic];
Hirose T&A(03) [4D analog of torus links]; Bodecker & Hornig PRL(04)
[for
triples of closed 2-forms].
@ Related topics: Jacobsen & Zinn-Justin mp/01 [enumeration];
Chernov & Rudyak CMP(08) [of spacetime manifolds, causality and linking]; > s.a. Ribbons.
> In physics:
see quantum systems.
Linkages
@ References: Tamburino & Winicour PR(66); Winicour JMP(68); Bramson PRS(75); Geroch & Winicour
JMP(81); Ashtekar & Winicour JMP(82).
Linking Numbers > see Link Theory; topological field theories.
Liouville Equation / Theory > s.a. 2-dimensional
gravity.
@ General references: Chambré JCP(52);
Matsuno JMP(87);
Teschner
CQG(01)
[rev]; Nakayama IJMPA(04)ht-MS & IJMPA(04);
Jackiw TMP(06)ht/05 [2D,
Weyl symmetry]; Banerjee et al a0807 [diffeomorphism
anomaly]; Momeni & Afrazeh IJMPB-a0904 [rev].
@ Quantum: Bershadsky & Klebanov PRL(90)
[path-integral quantization]; Jorjadze & Weigt
NPB(01)ht [Moyal
quantization]; Menotti JPCS(06)ht/05
[and semiclassical].
@ Generalizations: Tarasov Chaos(04)nl.CD/03 [fractional].
@ Related topics: Ferrari & Paturej PLB(08)mp/06 [and
Brownian motion].
Liouville Structure
* Idea: A structure
isomorphic to a cotangent vector fibration; An essential
ingredient of every variational formulation of a physical theory.
@ References: Tulczyjew & Urbanski a0806.
Liouville Theorem > see phase space.
Lippmann-Schwinger Equation
@ References: de la Madrid JPA(06)qp,
JPA(06)qp [rigged
Hilbert space approach].
Lipschitz Condition > s.a. analysis;
distance; distances
between metrics.
$ Locally Lipschitz real
function:
A function f on an open set O
R is
said to be locally Lipschitz if, for each open set U
O with
compact closure, there is some constant K such that (we use the Euclidean
norm in Rn)
for all x, y
U, |f(x)–f(y)|
K |x–y|
.
* Remark: A
"spacetime interpretation" is that the graph of the function is
a spacelike hypersurface in flat 2D space, with speed of light 1/K.
$ For a map between manifods:
Similarly, a map f of two manifolds
is
locally Lipschitz or C1– if the coordinates
of f(p)
are locally Lipschitz functions of those of p.
$ For a map between metric
spaces:
If (X, dX) and
(Y, dY) are metric
spaces, f : X → Y is
Lipschitz if
K such
that
for all x, y
X, dY(f(x), f(y))
K dX(x,y)
.
$ Bi-Lipschitz map between metric spaces: There exist two constants K, K' such that
for all x, y
X, K' dX(x,y)
dY(f(x),
f(y))
K dX(x,y)
.
Lipschitz Distance > see distance between metrics.
Liquid Matter > see condensed-matter physics; crystals [liquid crystals].
Little Group
@ Applications: Kim cm/96-in, ht/01-in
[particle symmetries].
@ Special cases: Banerjee et al MPLA(01)
[Maxwell-Chern-Simons, as gauge generator]; Scaria & Chakraborty CQG(02)ht [linearized
gravity, as gauge generator]; Lindner et al JPA(03)ht [for
massless particles].
Local Group, Local Void > see milky way galaxy
Local Pseudogroup of Transformations of a Manifold > see differentiable maps.
Locale
@ References: Pultr in(88).
Locality, Localizability > s.a. locality in quantum mechanics and in quantum field theory.
Locally Convex Topological Vector Space > see vector spaces.
Lock and Key Paradox > see special relativistic kinematics.
Loewner Equation > s.a. Scaling (relevant for scale-invariant
problems).
@ References: Kager et al JSP(04)mp/03 [solutions];
Kager & Nienhuis JSP(04)mp/03 [stochastic
evolution]; Gruzberg & Kadanoff
JSP(04).
Logarithm > see asymptotic flatness [logarithmic transformations]; entropy [deformed log's].
London's Equations > see electricity.
Long Line > see paracompact.
Longevity > see Doomsday Argument.
Loop Diagram > see quantum field theory formalism.
Loop Quantum Gravity > s.a. quantum
gravity in the connection representation
* Idea: The name given
to an approach to quantum gravity that originated with loop-based solutions of
the connection representation of canonical quantum
gravity and the of loop representation of quantum gravity; The
name has stuck despite the fact that states of quantum gravity in this approach
are now based on spin networks or spin-foam models.
Lorentz Equations
* Diffusionless: They
correspond physically to diffusionless convection.
@ Diffusionless: Huang PLA(03) [periodic and homoclinic orbits].
Lorentz Force > s.a. classical
particles; the gravitational one arises in gravitomagnetism.
* Idea: The force felt by a charged particle moving in an electromagnetic
field.
* Non-relativistic version:
Given by Fem = q (E + v
B)
.
* Relativistic version: If d
=
dt (1–v2)1/2 is
the proper
time interval,
m d2xa/d
2
= e Fab dxb/d
.
@ References: Buitrago EJP(95)-a0901 [and geometry of Minkowski space]; van Drie mp/00 [geometric, in terms of connections]; Buitrago & Hajjawi JMP(07)-a0901 [extended to spinors].
Lorentz Gauge > the correct spelling is Lorenz Gauge.
Lorentz Group > s.a. modifications and violation [theory]; phenomenology and tests.
Lorentz-Abraham Model > see particle models.
Lorentz-Dirac Equation / Force > see self-force.
Lorentz-FitzGerald
Contraction > s.a. kinematics of special
relativity.
* Idea: Objects moving
with velocity v are contracted in the direction of motion
by L(v) = L0 /
.
* And experiment:
It predicts a fringe shift in a Michelson interferometer upon a change
in speed wrt the ether (although not upon rotating the apparatus); this
is not observed.
@ References: Lorentz Nat(21); in Panofsky & Phillips
62, p278–279;
Brown AJP(01)oct-gq [history];
Martínez SHPMP(07);
Barceló & Jannes FP(08)-a0705 [in
condensed matter analogs of Lorentzian geometry].
Lorentzian Geometry / Metric / Structure
Lorenz Gauge > see gauge choices.
Lorenz System / Attractor
* Chaotic nature: The mechanism leading to chaotic behavior in the Lorenz system
is well understood; Homoclinic connections induce a strange invariant
set around the zero fluid motion stationary point, associated with
a Smale horseshoe.
@ References: Luzzatto et al CMP(05)m.DS/04 [attractor,
mixing nature]; Álvarez-Ramírez et al PLA(05)
[control by destruction of homoclinic
connections].
Loschmidt Echo
* Idea: A quantity M(t)
that measures the sensitivity of a quantum system to a perturbation; Defined
as the (squared) overlap of two wave functions evolved from the same initial
state but with slightly different
Hamiltonians;
Thus, it also serves as a quantification of irreversibility in quantum mechanics,
and has been extensively studied in connection
with the problems of quantum chaos, quantum computation and decoherence.
@ References: Wisniacki PRE(03)nl/02;
Cucchietti et al PRL(03)
[and decoherence/purity];
Cucchietti qp/04-PhD
[chaotic systems]; Combescure & Robert AHP(07)qp/05 [semiclassical
limit]; Gorin et al PRP(06)
[and fidelity decay]; Ares & Wisniacki a0908.
Lounesto Classification > see spinors.
Lovász Number > see graph.
Love Number > s.a. multipoles [black-hole
polarizability].
* Idea: A tidal Love
number relates the mass multipole moment created by tidal forces on a spherical
body to the applied tidal field.
@ References: Binnington & Poisson PRD(09)-a0906 [relativistic
theory].
Lovelock Gravity > s.a. higher-order
gravity.
* Idea: A theory with
higher-order curvature terms, which are
considered important for the low-energy action of string theories; Lovelock
terms in the action consist of the dimensionally-extended Euler densities,
polynomial scalar densities in the Riemann curvature tensor with the property
that their Euler-Lagrange derivatives contain derivatives
of the metric only up to second order (generic polynomial
scalar densities lead to Euler-Lagrange equations with derivatives of the
metric of order four); The theory is free from ghosts.
@ General references: Deruelle & Fariña-Busto PRD(90);
Müller-Hoissen
NPB(90);
Cnockaert & Henneaux CQG(05)ht [and
BRST cohomology]; Charmousis LNP(09)-a0805
[and brane world and black holes]; Canfora et al PRD(09)-a0812 [spontaneous
compactification, 4D general
relativity with small cosmological constant]; Bogdanos PRD-a0902 [scalar
densities, diagrammatic
techniques]; Willison PRD-a0904 [and
Weyl's tube formula].
@ Black holes: Dehghani & Pourhasan PRD(09)-a0903 [instability]; Cai
et al a0911 [vanishing mass and entropy]; > s.a. Birkhoff's
Theorem; black
holes
in
modified
theories [including
Lovelock-Born-Infeld].
@
Black-hole thermodynamics: Cai PLB(04)ht/03;
Aiello et al CQG(05)gq [+
Hoffmann-Infeld electromagnetism]; Correa-Borbonet BJP(05)ht [entropy];
Cai & Ohta PRD(06)ht [pure
Lovelock gravity].
@ Other solutions: Crisóstomo et al PRD(04)ht [collapsing
thin shells, Hamiltonian]; Willison gq/05-PhD
[hypersurfaces and branes]; Nozawa & Maeda CQG(06)gq/05 [collapse,
final fate]; Dehghani & Dayyani
PRD(09)-a0903 [wormholes];
Dehgani & Farhangkhah PLB(09)-a0904; > s.a.
bianchi I spacetimes.
Lovelock Identity > see tensor.
Lovelock Tensor
@ And curvature: Briggs gq/96 [quintic],
gq/97 [quartic],
gq/98 [more
general]; > s.a. tensor [identities].
Lowering Operator > essentially the same as annihilation operator; s.a. Ladder Operators.
LSZ Formalism
* Idea: A method of reducing
S-matrix elements to expressions given in terms of Green functions.
@ References: in Bjorken & Drell 65, #16.7.
Lukash Metric > see bianchi models [VIIh].
Luminosity Distance in Astronomy > see cosmological expansion.
Luminosity in High-Energy Physics
* Idea: The number
of interactions per unit cross section and unit time; A measure of beam intensity
and collimation.
Lump > see field theory [localized configuration].
Lunar Ranging > see tests of general relativity with orbits.
Luttinger-Liquid Theory
* Idea: The cornerstone
for the description of one-dimensional
materials; In it, an electron that carries both spin and charge cannot exist
as a well-defined particle: It splits into two collective excitations, one
carrying spin but not charge (the spinon), the other carrying charge but not
spin (the holon).
@ References: Giamarchi Phy(09) [viewpoint on electron transport results].
Lutzky's Theorem > see symmetries.
Lyra Geometry > s.a. bianchi
I models; other bianchi models; black holes in modified
theories.
@ Cosmology: Rahaman et al IJMPD(02)gq/07 [inhomogeneous
models].
main page – abbreviations – journals – comments – other
sites – acknowledgements
send feedback and suggestions to bombelli at olemiss.edu – modified
7 nov 2009