In
mathematics
Mathematics is an area of knowledge that includes the topics of numbers, formulas and related structures, shapes and the spaces in which they are contained, and quantities and their changes. These topics are represented in modern mathematics ...
, a Lie superalgebra is a generalisation of a
Lie algebra
In mathematics, a Lie algebra (pronounced ) is a vector space \mathfrak g together with an Binary operation, operation called the Lie bracket, an Alternating multilinear map, alternating bilinear map \mathfrak g \times \mathfrak g \rightarrow ...
to include a Z
2 grading. Lie superalgebras are important in
theoretical physics
Theoretical physics is a branch of physics that employs mathematical models and abstractions of physical objects and systems to rationalize, explain and predict natural phenomena. This is in contrast to experimental physics, which uses experim ...
where they are used to describe the mathematics of
supersymmetry
In a supersymmetric theory the equations for force and the equations for matter are identical. In theoretical and mathematical physics, any theory with this property has the principle of supersymmetry (SUSY). Dozens of supersymmetric theories e ...
. In most of these theories, the ''even'' elements of the superalgebra correspond to
boson
In particle physics, a boson ( ) is a subatomic particle whose spin quantum number has an integer value (0,1,2 ...). Bosons form one of the two fundamental classes of subatomic particle, the other being fermions, which have odd half-integer s ...
s and ''odd'' elements to
fermion
In particle physics, a fermion is a particle that follows Fermi–Dirac statistics. Generally, it has a half-odd-integer spin: spin , spin , etc. In addition, these particles obey the Pauli exclusion principle. Fermions include all quarks an ...
s (but this is not always true; for example, the
BRST supersymmetry is the other way around).
Definition
Formally, a Lie superalgebra is a nonassociative Z
2-
graded algebra
In mathematics, in particular abstract algebra, a graded ring is a ring such that the underlying additive group is a direct sum of abelian groups R_i such that R_i R_j \subseteq R_. The index set is usually the set of nonnegative integers or the se ...
, or ''
superalgebra
In mathematics and theoretical physics, a superalgebra is a Z2-graded algebra. That is, it is an algebra over a commutative ring or field with a decomposition into "even" and "odd" pieces and a multiplication operator that respects the grading.
Th ...
'', over a
commutative ring
In mathematics, a commutative ring is a ring in which the multiplication operation is commutative. The study of commutative rings is called commutative algebra. Complementarily, noncommutative algebra is the study of ring properties that are not sp ...
(typically R or C) whose product
·, · called the Lie superbracket or supercommutator, satisfies the two conditions (analogs of the usual
Lie algebra
In mathematics, a Lie algebra (pronounced ) is a vector space \mathfrak g together with an Binary operation, operation called the Lie bracket, an Alternating multilinear map, alternating bilinear map \mathfrak g \times \mathfrak g \rightarrow ...
axioms, with grading):
Super skew-symmetry:
:
The super Jacobi identity:
:
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where ''x'', ''y'', and ''z'' are pure in the Z
2-grading. Here, ">''x''"> denotes the degree of ''x'' (either 0 or 1). The degree of [x,yis the sum of degree of x and y modulo 2.
One also sometimes adds the axioms
for ">''x''"> = 0 (if 2 is invertible this follows automatically) and
for , ''x'', = 1 (if 3 is invertible this follows automatically). When the ground ring is the integers or the Lie superalgebra is a free module, these conditions are equivalent to the condition that the Poincaré–Birkhoff–Witt theorem holds (and, in general, they are necessary conditions for the theorem to hold).
Just as for Lie algebras, the
universal enveloping algebra
In mathematics, the universal enveloping algebra of a Lie algebra is the unital associative algebra whose representations correspond precisely to the representations of that Lie algebra.
Universal enveloping algebras are used in the representati ...
of the Lie superalgebra can be given a Hopf algebra structure.
A
graded Lie algebra In mathematics, a graded Lie algebra is a Lie algebra endowed with a gradation which is compatible with the Lie bracket. In other words, a graded Lie algebra is a Lie algebra which is also a nonassociative graded algebra under the bracket oper ...
(say, graded by Z or N) that is anticommutative and Jacobi in the graded sense also has a
grading (which is called "rolling up" the algebra into odd and even parts), but is not referred to as "super". See
note at graded Lie algebra for discussion.
Properties
Let
be a Lie superalgebra. By inspecting the Jacobi identity, one sees that there are eight cases depending on whether arguments are even or odd. These fall into four classes, indexed by the number of odd elements:
# No odd elements. The statement is just that
is an ordinary Lie algebra.
# One odd element. Then
is a
-module for the action
.
# Two odd elements. The Jacobi identity says that the bracket
is a ''symmetric''
-map.
# Three odd elements. For all
,
.
Thus_the_even_subalgebra_
_of_a_Lie_superalgebra_forms_a_(normal)_Lie_algebra_as_all_the_signs_disappear,_and_the_superbracket_becomes_a_normal_Lie_bracket,_while_
_is_a_representation_of_a_Lie_algebra.html" "title=",b.html" ;"title=",[b,b">,[b,b = 0.
Thus the even subalgebra
of a Lie superalgebra forms a (normal) Lie algebra as all the signs disappear, and the superbracket becomes a normal Lie bracket, while
is a representation of a Lie algebra">linear representation
Representation theory is a branch of mathematics that studies abstract algebraic structures by ''representing'' their elements as linear transformations of vector spaces, and studies modules over these abstract algebraic structures. In essenc ...
Conditions (1)–(3) are linear and can all be understood in terms of ordinary Lie algebras. Condition (4) is nonlinear, and is the most difficult one to verify when constructing a Lie superalgebra starting from an ordinary Lie algebra (
).
for all ''x'' and ''y'' in the Lie superalgebra. (Some authors prefer the convention
.
and then extending by linearity to all elements. The algebra
together with the supercommutator then becomes a Lie superalgebra. The simplest example of this procedure is perhaps when
to itself. When
. With the Lie bracket per above, the space is denoted
on homotopy groups gives many examples of Lie superalgebras over the integers.
The
.
This gives two orthosymplectic (see below) invariants if we take the m z variables and n w variables to be non-commutative and we take the real and imaginary parts. Therefore, we have
:
SU(n/n)/U(1) A special case of the superunitary Lie algebras where we remove one U(1) generator to make the algebra simple.
OSp(''m''/2''n'') These are the
s. They have invariants given by:
:
for ''m'' commutative variables (''x'') and ''n'' pairs of anti-commutative variables (''y'',''z''). They are important symmetries in
. It has dimension 17 and is a sub-algebra of OSp(9, 8). The even part of the group is O(3)×O(3)×O(3). So the invariants are:
:
.
F(4)
This exceptional Lie superalgebra has dimension 40 and is a sub-algebra of OSp(24, 16). The even part of the group is O(3)xSO(7) so three invariants are:
:
This group is related to the octonions by considering the 16 component spinors as two component octonion spinors and the gamma matrices acting on the upper indices as unit octonions. We then have
where ''f'' is the structure constants of octonion multiplication.
G(3)
This exceptional Lie superalgebra has dimension 31 and is a sub-algebra of OSp(17, 14). The even part of the group is O(3)×G2. The invariants are similar to the above (it being a subalgebra of the ''F''(4)?) so the first invariant is:
:
There are also two so-called strange series called p(''n'') and q(''n'').
Classification of infinite-dimensional simple linearly compact Lie superalgebras
The classification consists of the 10 series W(''m'', ''n''), S(''m'', ''n'') ((m, n) ≠(1, 1)), H(2m, n), K(2''m'' + 1, ''n''), HO(m, m) (''m'' ≥ 2), SHO(''m'', ''m'') (''m'' ≥ 3), KO(''m'', ''m'' + 1), SKO(m, m + 1; β) (''m'' ≥ 2), SHO ∼ (2''m'', 2''m''), SKO ∼ (2''m'' + 1, 2''m'' + 3) and the five exceptional algebras:
::E(1, 6), E(5, 10), E(4, 4), E(3, 6), E(3, 8)
The last two are particularly interesting (according to Kac) because they have the standard model gauge group SU(3)×SU(2)×U(1) as their zero level algebra. Infinite-dimensional (affine) Lie superalgebras are important symmetries in
. Specifically, the Virasoro algebras with
.
. In diagrammatic form:
: