Topics, B
Baby Universe > s.a. minisuperspace
quantum cosmology; multiverse.
@ References: Dijkgraaf et al PRD(06)ht/05,
IJMPD(06)
[in
string theory].
Bach Equation > see Conformal Gravity.
Bach Tensor > s.a. huygens
principle.
$ Def: For a Lorentzian
3-manifold with metric qab,
Babc := D[a (Rb]c –
R
qb]c)
.
* Applications: Used
to study the conformal symmetries of qab (vanishes
iff conformally flat).
@ References: in Ashtekar & Magnon CQG(84);
Glass CQG(01)gq [and
conserved current];
Álvarez
et al ht/02 [AdS-cft].
Back-Reaction > see self-force; semiclassical gravity.
Background Independence > see Covariance.
Bäcklund Transformation > see solitons.
Bag Model > s.a. casimir; Gravitational
Bag [different
kind]; QCD.
* Idea: A phenomenological model
for hadrons, originated at MIT, in which quark confinement is simulated by enclosing
them in a bag.
@ References: Chodos et al PRD(74)
[baryon structure]; Colanero
& Chu JPA(02)
[spherical, solution]; Lavenda ht/06 [thermodynamic
problem].
Baire Category Theorem > see distance.
Baker Map > s.a. chaotic
systems.
* Idea: A discrete chaotic
system.
@ Quantum: in Schack PRA(98)qp/97 [on
quantum computer]; Rubin & Salwen
AP(98)qp;
Schack PRA(98)
[and quantum computers]; Soklakov & Schack
PRE(00)qp/99;
Inoue et al qp/01,
JMP(02)qp/01 [semiclassical];
Tracy & Scott JPA(02)
[classical limit]; Lozinski
et al PRE(02)qp [irreversible];
Degli Esposti et al CMP(06)mp/04 [variance
and ergodicity]; Nonnenmacher & Anantharaman AHP(07)mp/05 [entropy
of semiclassical
measures]; Scherer et al PRD(06)
[coarse-grained evolution].
Ball > see sphere.
Banach Space > s.a. Degree
Theory; Orlicz Space; tensors [tensor
product].
$ Def: A complete normed vector space.
* Types: A Banach space E is
reflexive iff the canonical injection E → E** is onto.
* Examples: Any finite-dim'l
or Hilbert space; Lp for 1 < p <
;
C([0,1], R) with the Sup norm, not reflexive.
* Fréchet derivative:
The differential Df of a mapping f: X → Y between
(possibly infinite-dimensional) Banach spaces, defined by f(x+h) – f(x)
= Df(x) + R(h), where
R(h)
=
o(
h
);
Example: The operator giving the linearized version of a non-linear
pde.
@ References: Banach 32; Cirelli 72; Lindenstrauss & Tzafriri 77 [standard].
Barbour-Bertotti Model > see parametrized theories.
Bargmann Invariant > see phase.
Bargmann-Segal Representation / Transform > see representations of quantum theory.
Barker's Theory of Gravitation
@ References: Yepes & Domínguez-Tenreiro PRD(86)
[cosmological models].
Barnett Effect > see magnetism.
Barometric Formula > see gas.
Barrett-Crane Model > see spin foams.
Barycentric Coordinates > see simplex.
Baryogenesis > see early universe.
Baryons > see hadrons.
Base for a Topology
* Idea: A collection
of open sets generating the topology; every other one is the union of some
subcollection
of it.
Base Space > see bundle.
Basis for an R-Module > see module.
Batalin-Tyutin Quantization > see quantization of first-class constraints; quantum particles.
Bateman's Dual System > see oscillator.
Baum-Connes Conjecture > see deformation quantization.
Bayes Theory > see probability theory.
BCS Theory > s.a. superconductivity.
@ References: Hainzl et al CMP(08) [for general pair interactions].
Beable
* Idea: Within quantum
mechanics, theories of "beables" are, e.g, the theories of de Broglie,
Bohm, Bell, Vink, and also "modal" theories.
@ In quantum mechanics: Vink PRA(93);
Finkelstein PLA(96)qp/95 [measurement];
Clifton qp/97-in
[algebraic]; Elze JPA(08)
[symmetry of beables]; > s.a. hidden
variables.
Beal Conjecture > see conjectures.
Bell's Inequality > s.a. foundations of quantum mechanics.
Bell-Szekeres Spacetime > see gravitational wave solutions.
Berezinian
* Idea: The superdeterminant
of a supermetric.
@ References: Khudaverdian & Voronov mp/05 [formula].
Bergmann Manifold
@ References: Holm IJTP(90)
[connections].
Bergmann-Wagoner Theory > see scalar-tensor.
Bernoulli Equation
$ Def: The equation p +
![]()
v2 +
gy = constant.
Bernoulli Inequality > see inequalities.
Bernoulli Numbers
$ Def: The numbers Bn
that appear in the power series expansion
x / (ex – 1)
=
n=0infty Bn xn/n!
* History: First studied
by Faulhaber, but made popular by James Bernoulli.
> Online resources: CRC page.
Bernoulli Shift > see classical systems.
Berry's Phase > see geometric phase.
Berry-Hannay Model > see quantum systems.
Bertotti-Robinson Spacetime > see Robinson-Bertotti.
Bertrand's Theorem > see classical systems.
Bessel Transforms
@ References: Oberhettinger 72.
Beta Function > s.a. renormalization
group [in quantum field theory].
$ In mathematics: The function
B(x,y):= 2
0infty dt t2x–1 /
(t2 + 1)x+y , with
Re x >
0 and Re y > 0 .
related to the Gamma function by B(x,y)
=
(x)
(y)
/
(x+y).
Bethe Ansatz
* Idea: An ansatz to obtain the energy eigenstates of the one-dimensional version of
Heisenberg's model of interacting, localized spins.
@ References: Batchelor PT(07)jan
[history].
Bethe-Peierls Approximation > see ising model.
Bethe-Salpeter Equation > s.a. Salpeter
Equation [same?].
* Idea: Relativistic generalization
of the Schrödinger equation, used to describe bound states.
@ References: Nakanishi ed-PTPS(88)#95;
Karmanov & Carbonell EPJA(06)ht/05
[solution method].
Betti Numbers > s.a. euler classes.
* Idea: Topological
invariants representing roughly the number of independent p-dimensional
boundaryless surfaces which are not boundaries themselves; b0 is
the number of connected components and bk effectively
counts the number of k-dimensional
holes;
More specifically, the
number bk is the dimension
of the k-th de Rham cohomology group.
$ Def: The k-th Betti number of a manifold M, bk(M)
or Rk(M), is the
rank of the free part of the homology group Hk(M).
* Special cases: If there is no torsion subgroup, bk =
dim Hk(M);
If M is closed, Bp =
B4–p, B1 = B4 =
1; If M is simply connected, B1 = B3 = 0.
@ References: Yano & Bochner 53; Garvín & Lechuga T&A(03)
[elliptic space,
NP-hard]; Robins mp/06/PRE
[for Poisson-centered spheres of given radius].
BFV Formalism > see quantization of first-order constraints.
Bhabha Scattering
@ References: Bonciani & Ferroglia NPPS(06),
Becher & Melnikov JHEP(07)
[2-loop QED corrections].
Bi-Differential Calculus > see symmetry.
Bi-Hamiltonian Structure > see integrable systems; quantum systems and states; symmetry.
Bi-Local Fields > see types of field theories.
Bialgebras > see algebra.
Bianchi Classification > s.a. bianchi I; bianchi IX; bianchi models.
Bianchi Identities > see curvature.
Bicompact Space
* Idea: A compact Hausdorff
space; A bicompact space is T4.
Bicomplex
@ References: Dimakis & Müller-Hoissen IJMPB(00)ht,
JPA(00)nlin.SI [and
integrable models], JPA(01)
[and Bäcklund transformations].
Biconformal Spaces > see formulations of quantum mechanics.
Biconformal Vector Fields > see conformal structures.
Bidifferential Calculi > s.a. symmetries.
@ References: Chavchanidze mp/01 [and
non-Noether symmetries].
Bieberbach Conjecture > see conjectures.
Bieberbach Manifolds
@ References: Pfäffle JGP(00)
[Dirac spectrum].
Bifurcation Theory > s.a. Stability
Theory.
* History: 1879, Originated
with Poincaré; 1933, Developed by Andronov.
* Types: Pitchfork, Hopf
bifurcations.
@ General references: Iooss & Joseph 80; Chow & Hale 82 [standard
treatise]; Ruelle 89; Gaeta PRP(90);
Crawford
RMP(91).
@ Example: Johnson AJP(98) [unicycle].
Big Rip > see cosmology.
Big Trip
* Idea: A cosmological
process
thought to occur in the future by which the entire universe would be engulfed
inside a gigantic wormhole and might travel through it along space and time.
@ References: González-Díaz PLB(06)ht [viability];
Faraoni PLB(07)gq [unfounded
claims].
Bigravity > see under bimetric theory of gravity.
Bilinear Form
$ Def: A map B: V × V → R or
C, linear in both arguments, with V a vector space.
$ Hermitian form: A bilinear
form with B(x, y) =
B(y, x)*.
* Relationships: Any
quadratic function f : V → R determines
a bilinear form by B(u,v):=
[f(u+v) – f(u) – f(v)].
$ Strongly non-degenerate: A bilinear form (B: V × V → R,
considered as) B: V → V*, with V a vector
space,
is (strongly)
nondegenerate
if it is an
isomorphism
(1-1 and onto).
$ Weakly non-degenerate: B is
weakly nondegenerate if
it is only injective or 1-1;
This
means B(X, · ) = 0 iff X = 0.
Billiard > see classical systems; spectral geometry and quantum systems.
Bilocal Fields, Bilocality > see foundations of quantum mechanics; types of quantum field theories.
Binary Operation on a Set > see set.
Binary System > see dynamics of gravitating bodies; Two-Body Problem.
Binding Energy > see matter phenomenology in gravity.
Bing Topology
Binomial Coefficients
$ Def: The number of
ways to choose n different objects (unordered) out of k:
nCk
{n \choose k}:= n!
/ k! (n–k)!
.
* Properties: {n \choose m}
+ {n \choose m+1}
= {n+1 \choose m+1} ;
k =
0n (nCk)
= 2n ,
k =
0n k (nCk) =
n 2n–1 ,
k =
0n k2 (nCk)
= n (n + 1) 2n–2 , and
k =
0n (–1)k (nCk) =
0 .
* Remark: They get their
name from the fact that (a + b)n =
k =
0n (nCk) an–k bk .
@ References: Zhang DM(06)
[generalization of Calkin's identity]; Sun DM(08) [sums, and applications].
Binomial Distribution
$ Def: Given that a
property occurs with probability p per trial, the probability that
it occurs exactly n times out of N trials is
Pbin(n, N, p) = {N \choose n} pn (1–p)N–n .
* Cumulative binomial distribution:
The probability of it occurring j
n times, Pcb(n, N, p)
=
j Pbin(j, N, p)
for j = n, ..., N.
@ References: Kowalski JMP(00)
[generalized].
BIon
* Idea: A finite energy
solution of a non-linear field theory (> see, e.g., Born-Infeld)
with distributional sources (a soliton has no sources).
@ References: Gibbons CQG(99)ht/98 [from
branes]; Tamaki & Torii PRD(00)gq [Einstein-BI-dilaton],
PRD(01)gq [string-inspired].
Birefringence > see polarization.
Birkhoff's Theorem > s.a. spherical
symmetry in general relativity.
* Idea: The only vacuum,
spherically symmetric solution of Einstein's equation is static (and it is
the Schwarzschild metric).
* Generalizations: In
general relativity, it can be generalized to electrovacuum solutions, giving,
as unique spherically symmetric
solution, Reissner-Nordström (one cannot, however, generalize it to axisymmetric
solutions); Generalizes to other theories, but is violated in braneworld models,
such as Randall-Sundrum.
@ General references: Jebsen AMAF(21),
translation GRG(05);
in Birkhoff 23; in Hawking & Ellis 73;
Bondi & Rindler GRG(97)
[addendum re meaningful time coordinates]; Schmidt G&C(97)gq;
Abbassi
gq/98, gq/01 [more
solutions??]; Severa gq/02 [geometry];
Johansen & Ravndal GRG(06)phy/05 [history,
J T Jebsen]; Deser GRG(05)
[re Jebsen]; Deser & Franklin AJP(07)
[and t-independence in general relativity].
@ Higher-order gravity: Zegers JMP(05)gq [Lovelock];
Deser & Franklin CQG(05)gq
[with second-order field equations].
@ With cosmological constant: Rindler PLA(98)
[reformulation, Bertotti-Kasner as extra solution];
Ayón-Beato et al PRD(04)ht [2+1,
< 0].
@ For various theories: Venkateswarlu & Reddy ASS(89)
[scalar-tensor]; Brodbeck & Straumann
JMP(93) [Einstein-Yang-Mills];
Bronnikov & Melnikov
GRG(95)
[higher dimensions]; Schmidt G&C(97)gq [including
other signatures]; Cavaglià
ht/98-in
[quantum dilaton gravity]; Cavaglià G&C(99)gq [topologically
massive gravity]; Keresztes & Gergely a0712 [5D].
@ Consequences of non-validity: Dai et al a0709 [DGP model].
@ Other generalizations: Szenthe JGP(07).
Bistochastic Matrix > see matrices.
Bivector > s.a. types
of field theories [bivector
fields].
* Idea: An object of
the form u[avb],
representing the u-v
plane; The magnitude can be given by ua vb
u[a vb].
* In a Lorentzian metric:
The sign of the "magnitude" is related to whether the plane is spacelike,
timelike, or null.
Black-Body Radiation > see thermal radiation.
Black Holes > s.a. black hole solutions, thermodynamics; quantum black holes; [< part of gravitation and cosmology].
Black Tides > see black hole phenomenology.
Blandford-Znajek Effect > see black hole phenomenology.
Blazar > see black hole phenomenology; astrophysics; gamma-ray astronomy.
Bloch Ball / Sphere > see quantum systems.
Bloch Theory
* Application: Analyze
spectral properties of differential operators which are invariant under an
abelian group.
* Bloch's theorem:
Electron wave functions in the presence of a periodic potential (such
as the electric potential of a crystalline
lattice of atoms) are of the
form exp{
i kx} u(x),
where u(x) is periodic with the same period.
* Bloch oscillations:
A phenomenon that occurs when particles subject to a periodic potential are
exposed to an additional static force, say, an electric (or gravitational)
force in a single direction; The electrons then do not all move in the direction
of the force, but instead oscillate back and forth in place; > s.a. tests
of newtonian gravity.
@ References: Gruber JMP(01)mp/00 [non-commutative
generalization]; Bouda & Meziane IJTP(06)qp/07 [Hamilton-Jacobi
formulation].
Block Universe > see time.
BMS Group > see asymptotic flatness at null infinity.
Bochner Theorem
* Idea: A result on
measures in constructive quantum field theory.
@ References: in Gel'fand & Vilenkin 64; in Yamasaki 85.
Bode's Law > see Titius-Bode Law.
Bogoliubov Quasiparticle > see Quasiparticles.
Bogomolny Equation
* Idea: The equation B = D
one
gets in Yang-Mills-Higgs theories, minimizing the energy with the constraint
2 = C2,
whose solution gives a class
of monopoles.
* And self-duality:
If one considers
as
the 5th component of
A, the equation becomes the self-dual equation Fab =
abcd Fcd,
whose solutions are static self-dual monopoles, characterized by an
integer m; For m = 1, we have the Prasad-Sommerfied solutions.
@ References: Bogomolny SJNP(76); Coleman, Parke, Neveu & Sommerfield PRD(77).
Bogomol'ny Inequality > s.a. positive
energy theorems.
* Idea: A lower
bound on the mass of a monopole solution in a gauge theory in terms of its electric
and
magnetic charges.
@ For Kaluza-Klein monopoles: Lee & Sorkin CMP(88).
Bohm Metrics
* Idea: Infinite sequences
of inhomogeneous Einstein metrics on spheres and products of spheres of dimension
5
d
9.
@ References: Gibbons et al PRD(03).
Bohr
Compactification of R > s.a.
functions [almost periodic].
* Idea: A compact group
obtained as the dual of the real line endowed with the discrete topology;
Can be used as the configuration space for a non-standard, polymer representation
for the quantum theory of a system on the real line.
@ General references: Halvorson SHPMP(04)qp/01;
in Bratteli & Robinson 02.
@ And quantum mechanics of point particles: Ashtekar et al CQG(03)gq/02;
> s.a Polymer Representation of
Quantum Theory.
@ And quantum gravity / quantum cosmology:
Husain & Winkler PRD(04)gq/03;
Velhinho CQG(07)-a0704; > s.a. minisuperspace.
Bohr Magneton
* Idea: The constant
0 =
e
/2mc.
Bohr Model of the Atom > see history of quantum physics.
Bohr-Rosenfeld > see quantum measurement [quantum field theory].
Boltzmann Brains
@ References: Overbye NYT(08)jan.
Boltzmann Constant > see constants.
Boltzmann (Transport)
Equation > s.a. fluids [Navier-Stokes];
stochastic process.
* Approximations involved:
(i) Dilute gas, there are only binary collisions; (ii) Ignore the
walls of the container; (iii) Ignore the effect of the external force on
the collision cross section; (iv) Molecular
chaos, the velocity of a molecule is uncorrelated to its position.
* Chapman-Enskog method:
A successive approximations method used to find some solutions of the Boltzmann
equation.
@ General references: in Huang 63*; in Gorban & Karlin cm/03 [rev].
@ Solutions and techniques: in Huang 63 [Chapman-Enskog];
Kandrup ap/97 [collisionless,
t-independent]; Cercignani JSP(05)
[global, weak]; Yu JSP(06)
[Green's function]; Yang & Zhao JMP(06)
[energy method]; Bardos et al JSP(06)
[in half space].
@ Quantum: & Joichi, Matsumoto, Yoshimura; Singh & Srednicki
PRD(00)hp/99;
Yamamoto IJMPA(03)ap [fermions
in curved spacetime]; Chen CMP(06)
[as limit of random Schrödinger equation]; Breuer & Vacchini
a0707 [Monte
Carlo simulation].
@ Relativistic: Lucquiaud JMP(78);
Horwitz FP(95); Calogero JMP(04)mp [Newtonian
limit]; Noutchegueme et al GRG(05)gq,
& Dongo CQG(06)gq/05 [in
Bianchi I]; Takou & Noutchegueme gq/05 [in
flat FRW].
Bolzano-Weierstrass Theorem > see compactness.
Bondi Mass > see asymptotic flatness at null infinity.
Bondi-Sachs Metric > see gravitational wave solutions.
Bonnor / Bonnor-Swaminarayan Solutions > s.a. c-metric.
* Idea: Boost-rotation
symmetric spacetimes describing pairs of accelerating particles, possibly
connected to struts.
@ References: Podolsky & Griffiths GRG(01)gq/00 [null
limits]; Garecki CQG(05)gq/04 [energy-momentum].
Bonnor-Ward Spacetimes
@ References: Rosa & Letelier PLA(07)
[closed timelike geodesics, stability].
Boolean Algebra > s.a. logic.
$ Def: A ring R of
subsets of a space X, with X in R.
Boost > see kinematics of special relativity.
Bootstrap Theory
* Idea: An approach to
understanding elementary particles in hadronic physics that was very popular
in the 1960s (one of the main proponents was Geoffrey Chew), as an alternative
to quantum field theory.
@ References: Chew SA(64)apr; Redhead FP(05)
[overview, assessment].
Bordism
Borel Fixed Point Theorem > see fixed point theorems.
Borel Measure, Sigma-Field > s.a. ring.
* Idea: A positive
measure on Borel sets of a locally compact Hausdorff topological space.
$ Borel sets: The Borel
-field
of a topological space X is the one generated by the open (or the
closed) sets in X; An element of it is a Borel set.
Born Rule
* Idea: The statement
that
=
|
|2,
or in general that the probability of obtaining a certain eigenvalue of an
observable in a measurement is the
square modulus of the corresponding coefficient in the expansion
of the state in eigenvectors.
@ References: Born ZP(26);
Zurek PRL(03),
Schlosshauer & Fine FP(05)qp/03 ["envariance" derivation];
Valentini & Westman PRS(05)qp/04 [dynamical
origin, in pilot wave]; Mould qp/05 [replace
by probability current alone]; Brumer & Gong PRA(06)qp
[in quantum and classical mechanics]; Buniy et al PLB(06)ht [and
state space discreteness]; Landsman a0804 [mathematical
clarificaton of role].
Born-Oppenheimer Approximation > s.a. semiclassical
quantum gravity.
* Idea: An approximation
used in the quantum theory
of
molecules, in which ones divides the degrees of freedom into "heavy" ones, the
nuclei,
and
"light"ones,
the
electrons.
Bose-Einstein Condensation > s.a. atomic;
effective field theories; light; sound;
temperature; vacuum [fluctuation].
* Idea: A phase transition
of a gas of bosons consisting in the amalgamation of many bosonic atoms so
cold and dense (chilled to nearly 0 K) that they act
as a single quantum state, essentially a single "superparticle";
This occurs when T is so low that the atoms' de Broglie wavelength
becomes comparable to the distance between them; Similar to Cooper
pairs in superconductors.
* History, theory: Started
with S N Bose's letter to Einstein in 1924, after his paper was rejected by
Philosophical Magazine; Einstein extended the ideas to massive particles in
1925; Viewed with skepticism (how can you have condensation in an ideal gas,
without forces; No applications, ...) until 1938, when F London proposed it
to explain He superfluidity, discovered in 1928.
* History, experiment:
First produced in 1995, with
5 million Rb atoms, directly observable; The 2001 Nobel prize for physics
was given for Bose-Einstein condensation in dilute gases of alkali atoms; 1998,
For H atoms (at T
40
K, with
about 100 million atoms); 2003, Observed in Ytterbium, which differs from most
of the elements that have previously been condensed because it has two valence
electrons
rather than one, and can be prepared in a non-magnetic state; 2005, Observed
in Chromium, which has a very large magnetic dipole moent.
* Properties: Enormous
indices of refraction.
@ Books: Pitaevskii & Stringari 03 [r PT(04)oct]; Annett
04
[intro].
@ General references: Scharf AJP(93);
Cornell & Wieman SA(98)mar; Ketterle PT(99)dec
[experiments]; Burnett et al PT(99)dec
[theory]; Collins
SA(00)dec; Yukalov PLA(06)
[self-consistent theory]; Schlein a0704-in
[dynamics].
@ Specific types of gases: news pn(95)jul, pn(95)aug, pn(98)nov, pn(99)jun,
Bradley et al PRL(95)
[atoms];
Wynar
et al Sci(00)feb
+ pn(00)feb
[Rb2 molecules];
Hall AJP(03)RL
[trapped dilute gases]; Takasu et
al PRL(03)
+ pw(03)jul
[in
Yb]; news pw(05)mar
[chromium]; Grether et al PRL(07) [relativistic ideal
Bose gas].
@ Related topics:
Reichel SA(05)feb [and microchips]; Dorlas
et
al mp/05 [and
long cycles]; Lye et al PRL(05)
[in a random potential]; Schützhold PRL(06)
[accurate phonon detection]; Damski & Zurek PRL(07)
[spin-1, quantum phase transition]; news pw(08)may [use to measure small forces].
> Gravity-related
topics: see black hole analogs; lorentz
symmetry breaking; quantum field theory effects; matter
in quantum garvity; types of dark matter.
Bosons > s.a. particle
statistics.
@ Related effects: Gogolin et al PRL(08)
[solution to three-body problem, including Efimov trimers]; > s.a. atomic
physics, Chirality.
Boson Star > see astronomical objects.
Bosonization > s.a. particle
statistics; types
of field theories.
@ References: Liguori & Mintchev NPB(98)ht/97 [on
the half-line]; Ilinskaia & Ilinski
cm/98-in;
Dhar & Mandal PRD(06)ht [non-relativistic
fermions on S1]; Kanakoglou & Daskaloyannis
mp/07-in
[and parastatistics].
Bott's Periodicity Theorem
* Idea: A theorem on
periodicities in
q(G) for Lie groups (> see homotopy).
@ References: in Milnor 73 [last chapter].
Boulware Vacuum > see quantum field theory in curved backgrounds.
Bounce > see relativistic cosmological models.
Bound State > see atomic physics; types of quantum states.
Boundary > s.a. boundaries
in field theory; spacetime
boundary.
$ In homology: A q-chain c such
that c =
(c'), for some (q+1)-chain c'.
$ In topology: The
boundary of a subset S
X is
its closure minus its
interior, S · or
S:=
\ovr S – int(S).
Boundary Conditions > see boundaries in field theory; electromagnetism; quantum cosmology.
Boundary Value Problems > see Dirichlet, Neumann and Robin problem; laplace equation.
Bounded Convergence Theorem
* Idea: Under appropriate
circumstances, the integral of a limit function, is the limit of the integrals.
Bounded Operator > see operator theory.
Bounded Variation > see functions.
Boyer-Lindquist Coordinates > see kerr metric.
BPS Solutions > see black hole solutions, and black holes in modified theories.
Bradyon
* Idea: A slower-than-light particle (> aot a tachyon).
Braided Geometry > see geometry.
Braids
* Idea: A braid is a
set of n strings stretching between two parallel planes.
* Application: They
have been used as tools in the calculation of knot and link invariants; > s.a.
3D general relativity; composite
models.
@ Braid group: Cappuccio & Guadagnini PLB(90) [statistics]; > s.a. group
types.
@ Invariants: Berger LMP(01); Nechaev & Voituriez NPB(05) [3-strand, Brownian].
Brane World > s.a. brane cosmology.
Bravais Lattice > see crystals.
Bremsstrahlung > see radiation.
Brick Wall Model > see black hole entropy.
Brieskorn Sphere > see 3-manifolds.
Brillouin Zone > see cell complex.
Brillouin-Wigner Perturbation Expansion
@ References: see Ziman 69, pp 55–56.
Brinkman's Theorem > see types of spacetimes [Einstein spaces].
Brouwer Theorem > s.a. fixed-point
theorems.
$ Def: The unit sphere Sn in En is not a retract of the
closed unit ball Bn which it bounds.
Brown Dwarfs > s.a. extrasolar
planets.
* Idea: Substellar objects
that can be seen through the release of some of their internal gravitational
energy; Their
masses are between 0.001 and 0.1 MSun.
* Consequences: They are a candidate for dark matter (Bahcall 1984).
* Observation methods: Look for methane lines in spectrum.
* Examples: Jupiter;
VB8B, first outside the solar system, M
10–50
MJup, T = 1360 K, R =
0.09 RSun); Gliese 229B,
first unambiguous sighting,
d
30 ly, M
20–50
MJup,
T < 1000
K [@ Nakajima et al Nat(95)nov].
@ I: PW(90)oct, 34–38; Martin et al AS(97), Basri SA(00)apr [discovery];
Mohanty & Jayawardhana SA(06)jan.
@ General references: Jameson & Hodgkin
CP(97);
Oppenheimer et al ap/98-in;
Chabrier ap/99-in
[physics].
Brudno Theorem
* Idea: A result in classical information theory, relating entropy rate and algorithmic
complexity per symbol.
@ References: Benatti et al CMP(06)
[quantum version, connecting von Neumann entropy rate and quantum Kolmogorov
complexity].
BTZ Spacetime > see 3D black holes.
Bubbles > see fluids; matter [soap].
Buchdahl Inequality > see astrophysics.
Buffon's Needle > see statistical geometry.
Bunch-Davies Vacuum > see quantum field theory in curved backgrounds.
Bundle [including Bundle Gerbes, Bundle Map]
Bures Metric > see mixed quantum states; riemannian geometry; types of distances.
Burgers Equation [@ wikipedia.]
* Idea: A partial differential equation used in fluid dynamics.
@ References: Kirsch & Simon mp/01 [forced,
approach to equilibrium]; Hamanaka & Toda JPA(03)
[non-commutative]; Bec & Khanin PRP(07)
[turbulence].
Burnside Ring of a Group > see ring.
Butcher Group > related to Hopf Algebras.
Butcher Series > see scalar field theory.
Main page – Abbreviations – Journals – Comments – Other
sites – Acknowledgements
Send feedback and suggestions to bombelli at olemiss.edu – Modified
16 jul 2008