In General > s.a. examples and representations.
$ Def: A Lie algebra A is a vector space on some field K,
with a Lie bracket [ , ]: A × A → A satisfying:
- Antisymmetry: [x, y]
= –[y, x],
for all x, y
A;
- Linearity: [
x, y]
=
[x, y],
[x+y, z]
= [x, z]
+ [y, z],
for all x, y, z
A,
for all
K;
- Jacobi identity: [x,
[y, z]]
+ [y, [z, x]]
+ [z, [x, y]] =
0, for all x, y, z
A.
* Structure constants: Given
a basis Ti for the L.a.,
they are defined in that basis by: [Ti, Tj]
= Ckij Tk.
@ General references: Jacobson 62; Serre 64; Kaplansky 71; Humphreys
72; Erdmann & Wildon 06 [II/III]; Hall 06; Goze a0805 [rev].
@ Space of Lie algebras: Ritter mp/03 [topology
and invariants]; Goze m.RA/06-ln
[classification, deformations and rigidity]; Shirokov a0705 [classification
using Clifford algebras].
@ Related topics: Cariñena et al JPA(94) [and Poisson tensors]; Paal CzJP(03)mp-in
[and Moufang loops]; Sabinin 04 [mirror
symmetry].
Invariants > s.a. Casimir
Operator; Weil Homomorphism.
* Result: All invariants of a Lie algebra are obtained by expanding
the m × m determinant
det(t I + ai Ti)
=
r=0m Pm–r(ai) tr
in powers of t, and substituting Ti to
get the polynomials Pm–r
(Ti).
@ References: Di Francesco & Zinn-Justin mp/05 [1-parameter
family of vector-valued polynomials]; Boyko et al JPA(06)mp [moving
frame method].
Subsets, Operations and Other Structure > s.a. Cartan
Subalgebra; Center.
* Metric: A metric can be defined on a Lie algebra by
gij = Ckli Clkj ;
if the Lie algebra is semisimple, this metric is non-degenerate.
* Deformations and contractions: They
are mutually opposite procedures, but whereas for every contraction there exists
a reverse deformation, the converse is not true in general; For examples, global
deformations of the Witt, Virasoro, and affine Kac-Moody algebras allow one
to retrieve Lie algebras of Krichever-Novikov type; > s.a. deformation
quantization.
@ Extensions: Landi & Marmo in(89) [and gauge theories]; Forte & Sciarrino JMP(06)ht/05.
@ Contractions: Fialowski & de Montigny JPA(05), Sigma(06)m.RT [and
contractions]; Nesterenko & Popovych JMP(06)mp;
Vitiello IJTP(08)
[and quantum field theory]; Doikou & Sfetsos a0904 [and central extensions].
@ Other operations: de Azcárraga et al NPB(03),
Izaurieta et al JMP(06)ht [expansion];
Nurowski
JGP(07)
[deformations from 2-forms]; > s.a. Central
Extension.
Of a Lie Group G > s.a. conformal
group [SO(3,2)];
lie group; lorentz; poincaré;
SU(2).
$ Def: The vector space
of left-invariant vector fields on the Lie group G,
together
with Lie bracket multiplication.
* Examples: (special group)
implies (traceless algebra):
| GL(n, R), real matrices; GL(n, C), complex matrices; SL(n, R), real traceless matrices; SL(n, C), complex traceless matrices; |
O(n), real antisymmetric matrices; SO(n), real antisymmetric matrices; U(n), complex antihermitian matrices; SU(n), complex antihermitian matrices. |
* SU(1,1): Generators Ka, a =
1, 2, 3, with [K1, K2]
= –i
K3,
[K2, K3]
= i
K1,
[K3, K1]
= i
K2.
* SO(2,1), 1+1 de Sitter: Generators Pa, a =
1, 2, and
,
with
[Pa, Pb]
= k
ab
and
[
, Pa]
=
ab Pb.
@ References: Su qp/06-in
[su(N), Cartan decomposition].
Infinite-Dimensional > s.a. Surfaces [deformations].
* Examples: > see
Kac-Moody, Virasoro,
and Witt Algebra.
* History: They first appeared in 1909 in a paper by Cartan.
* Applications: The main
ones in physics are in gauge theories, where
the
locality of the gauge transformations causes the infinite-dimensionality,
and
in the study of diffeomorphism groups (for even very simple spaces like S1!).
@ References: Cornwell 89; Kac 90; Wakimoto 01.
Other Types and Related Concepts > s.a. Drinfeld
Doubles; Fusion
Rules [affine]; knot
invariants [and quantum groups].
* Simple: For each simple
Lie algebra
,
one can construct a Hopf
algebra Uq(
),
and a polynomial link invariant.
$ S theorem: Any invariant of a compact semisimple Lie algebra is symmetric
wrt the reflections which generate the discrete Weyl group of the algebra.
@ General references: Gruber & O'Raifeartaigh JMP(64) [S theorem]; Cahn 84.
@ Bialgebras:
Golubchik & Sokolov TMP(06) [and solutions of Yang-Baxter equation].
Generalizations > s.a. poisson
structure; Quantum
Algebra.
* Soft Lie algebra:
One with structure functions rather than structure constants, e.g., the 7-sphere.
* Lie 2-algebra:
A"categorified" version of a Lie algebra, a category equipped with
structures analogous those of a Lie algebra, for which
the usual laws hold up to isomorphism.
@ Lie algebroids: Iglesias & Marrero; Cattaneo LMP(04)m.SG/03 [integration];
de León et al m.DG/04 [Hamiltonian
mechanics]; Landsman JGP(06)mp/05
[in physics, rev]; > s.a. yang-mills theories.
@ Superalgebras: Zhang & Gould JMP(05)m.QA/04 [representations
of gl(2|2)]; Faux & Gates PRD(05)
[Adinkras graphical technique]; Gotz et al JA(07)ht/05 [representations
of sl(2|1)].
@ Lie n-algebras:
Baez et al m.QA/05 [2-algebras,
loop groups and String(n)]; Papadopoulos CQG(08)
[structure constants]; Figueroa-O'Farrill JMP(08)
[with Lorentzian inner product], a0904 [3-algebras,
deformations].
@ Other types: Majid JGP(94)
[braided, quantum]; Burde CEJM(06)mp/05 [left-symmetric
or pre-Lie
algebras]; Ovsienko a0705,
AIP(08)-a0810 [Lie
antialgebras]; Goze et al a0909 [n-Lie
algebras].
In Physics > s.a. algebras [including
quantum algebra]; Feynman Diagram; lagrangian
dynamics [conserved currents].
@ Texts: Hermann 70; Georgi 82; Azcárraga & Izquierdo 95;
Fuchs & Schweigert
97; Prakash 03 [including
-dimensional].
@ Specific systems: McLachlan & Ryland mp/02/JMP
[classical mechanics].
@ Deformations: Chryssomalakos & Okon IJMPD(04)ht [quantum
relativistic kinematic algebra]; > s.a. deformation
quantization.
@ Lie-algebra cohomology and applications: de Azcárraga et al RRAC(01)phy/98-in.
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sep
2009