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Lie superalgebra

The notion of ${\displaystyle \mathbb {Z} /2\mathbb {Z} }$ grading used here is distinct from a second ${\displaystyle \mathbb {Z} /2\mathbb {Z} }$ grading having cohomological origins. A graded Lie algebra (say, graded by ${\displaystyle \mathbb {Z} }$or${\displaystyle \mathbb {N} }$) that is anticommutative and has a graded Jacobi identity also has a ${\displaystyle \mathbb {Z} /2\mathbb {Z} }$ grading; this is the "rolling up" of the algebra into odd and even parts. This rolling-up is not normally referred to as "super". Thus, supergraded Lie superalgebras carry a pairof${\displaystyle \mathbb {Z} /2\mathbb {Z} }$‑gradations: one of which is supersymmetric, and the other is classical. Pierre Deligne calls the supersymmetric one the super gradation, and the classical one the cohomological gradation. These two gradations must be compatible, and there is often disagreement as to how they should be regarded.^[1]

Formally, a Lie superalgebra is a nonassociative Z₂-graded algebra, or superalgebra, over a commutative ring (typically RorC) whose product [·, ·], called the Lie superbracketorsupercommutator, satisfies the two conditions (analogs of the usual Lie algebra axioms, with grading):

Super skew-symmetry:

${\displaystyle [x,y]=-(-1)^{|x||y|}[y,x].\ }$

The super Jacobi identity:^[2]

${\displaystyle (-1)^{|x||z|}[x,[y,z]]+(-1)^{|y||x|}[y,[z,x]]+(-1)^{|z||y|}[z,[x,y]]=0,}$

where x, y, and z are pure in the Z₂-grading. Here, |x| denotes the degree of x (either 0 or 1). The degree of [x,y] is the sum of degree of x and y modulo 2.

One also sometimes adds the axioms ${\displaystyle [x,x]=0}$ for |x| = 0 (if 2 is invertible this follows automatically) and ${\displaystyle [[x,x],x]=0}$ 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 of the Lie superalgebra can be given a Hopf algebra structure.

Lie superalgebras show up in physics in several different ways. In conventional supersymmetry, the even elements of the superalgebra correspond to bosons and odd elements to fermions. This corresponds to a bracket that has a grading of zero:

${\displaystyle |[a,b]|=|a|+|b|}$

This is not always the case; for example, in BRST supersymmetry and in the Batalin–Vilkovisky formalism, it is the other way around, which corresponds to the bracket of having a grading of -1:

${\displaystyle |[a,b]|=|a|+|b|-1}$

This distinction becomes particularly relevant when an algebra has not one, but two graded associative products. In addition to the Lie bracket, there may also be an "ordinary" product, thus giving rise to the Poisson superalgebra and the Gerstenhaber algebra. Such gradings are also observed in deformation theory.

Let ${\displaystyle {\mathfrak {g}}={\mathfrak {g}}_{0}\oplus {\mathfrak {g}}_{1}}$ 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:^[3]

1. No odd elements. The statement is just that ${\displaystyle {\mathfrak {g}}_{0}}$ is an ordinary Lie algebra.
2. One odd element. Then ${\displaystyle {\mathfrak {g}}_{1}}$ is a ${\displaystyle {\mathfrak {g}}_{0}}$-module for the action ${\displaystyle \mathrm {ad} _{a}:b\rightarrow [a,b],\quad a\in {\mathfrak {g}}_{0},\quad b,[a,b]\in {\mathfrak {g}}_{1}}$.
3. Two odd elements. The Jacobi identity says that the bracket ${\displaystyle {\mathfrak {g}}_{1}\otimes {\mathfrak {g}}_{1}\rightarrow {\mathfrak {g}}_{0}}$ is a symmetric ${\displaystyle {\mathfrak {g}}_{1}}$-map.
4. Three odd elements. For all ${\displaystyle b\in {\mathfrak {g}}_{1}}$, ${\displaystyle [b,[b,b]]=0}$.

Thus the even subalgebra ${\displaystyle {\mathfrak {g}}_{0}}$ of a Lie superalgebra forms a (normal) Lie algebra as all the signs disappear, and the superbracket becomes a normal Lie bracket, while ${\displaystyle {\mathfrak {g}}_{1}}$ is a linear representationof${\displaystyle {\mathfrak {g}}_{0}}$, and there exists a symmetric ${\displaystyle {\mathfrak {g}}_{0}}$-equivariant linear map ${\displaystyle \{\cdot ,\cdot \}:{\mathfrak {g}}_{1}\otimes {\mathfrak {g}}_{1}\rightarrow {\mathfrak {g}}_{0}}$ such that,

${\displaystyle [\left\{x,y\right\},z]+[\left\{y,z\right\},x]+[\left\{z,x\right\},y]=0,\quad x,y,z\in {\mathfrak {g}}_{1}.}$

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 (${\displaystyle {\mathfrak {g}}_{0}}$) and a representation (${\displaystyle {\mathfrak {g}}_{1}}$).

A^∗ Lie superalgebra is a complex Lie superalgebra equipped with an involutive antilinear map from itself to itself which respects the Z₂ grading and satisfies [x,y]^* = [y^*,x^*] for all x and y in the Lie superalgebra. (Some authors prefer the convention [x,y]^* = (−1)^|x||y|[y^*,x^*]; changing * to −* switches between the two conventions.) Its universal enveloping algebra would be an ordinary ^*-algebra.

Given any associative superalgebra ${\displaystyle A}$ one can define the supercommutator on homogeneous elements by

${\displaystyle [x,y]=xy-(-1)^{|x||y|}yx\ }$

and then extending by linearity to all elements. The algebra ${\displaystyle A}$ together with the supercommutator then becomes a Lie superalgebra. The simplest example of this procedure is perhaps when ${\displaystyle A}$ is the space of all linear functions ${\displaystyle \mathbf {End} ($V)} of a super vector space ${\displaystyle V}$ to itself. When ${\displaystyle V=\mathbb {K} ^{p|q}}$, this space is denoted by ${\displaystyle M^{p|q}}$or${\displaystyle M(p|q)}$.^[4] With the Lie bracket per above, the space is denoted ${\displaystyle {\mathfrak {gl}}(p|q)}$.^[5]

APoisson algebra is an associative algebra together with a Lie bracket. If the algebra is given a Z₂-grading, such that the Lie bracket becomes a Lie superbracket, then one obtains the Poisson superalgebra. If, in addition, the associative product is made supercommutative, one obtains a supercommutative Poisson superalgebra.

The Whitehead product on homotopy groups gives many examples of Lie superalgebras over the integers.

The super-Poincaré algebra generates the isometries of flat superspace.

The simple complex finite-dimensional Lie superalgebras were classified by Victor Kac.

They are (excluding the Lie algebras):^[6]

The special linear lie superalgebra ${\displaystyle {\mathfrak {sl}}(m|n)}$.

The lie superalgebra ${\displaystyle {\mathfrak {sl}}(m|n)}$ is the subalgebra of ${\displaystyle {\mathfrak {gl}}(m|n)}$ consisting of matrices with super trace zero. It is simple when ${\displaystyle m\not =n}$. If ${\displaystyle m=n}$, then the identity matrix ${\displaystyle I_{2m}}$generates an ideal. Quotienting out this ideal leads to ${\displaystyle {\mathfrak {sl}}(m|m)/\langle I_{2m}\rangle }$ which is simple for ${\displaystyle m\geq 2}$.

The orthosymplectic Lie superalgebra ${\displaystyle {\mathfrak {osp}}(m|2n)}$.

Consider an even, non-degenerate, supersymmetric bilinear form ${\displaystyle \langle \cdot ,\cdot \rangle }$on${\displaystyle \mathbb {C} ^{m|2n}}$. Then the orthosymplectic Lie superalgebra is the subalgebra of ${\displaystyle {\mathfrak {gl}}(m|2n)}$ consisting of matrices that leave this form invariant:$${\displaystyle {\mathfrak {osp}}(m|2n)=\{X\in {\mathfrak {gl}}(m|2n)\mid \langle Xu,v\rangle +(-1)^{|X||u|}\langle u,Xv\rangle =0{\text{ for all }}u,v\in \mathbb {C} ^{m|2n}\}.}$$ Its even part is given by ${\displaystyle {\mathfrak {so}}($m)\oplus {\mathfrak {sp}}(2n)} .

The exceptional Lie superalgebra ${\displaystyle D(2,1;\alpha )}$.

There is a family of (9∣8)-dimensional Lie superalgebras depending on a parameter ${\displaystyle \alpha }$. These are deformations of ${\displaystyle D(2,1)={\mathfrak {osp}}(4|2)}$. If ${\displaystyle \alpha \not =0}$ and ${\displaystyle \alpha \not =-1}$, then D(2,1,α) is simple. Moreover ${\displaystyle D(2,1;\alpha )\cong D(2,1;\beta )}$if${\displaystyle \alpha }$ and ${\displaystyle \beta }$ are under the same orbit under the maps ${\displaystyle \alpha \mapsto \alpha ^{-1}}$ and ${\displaystyle \alpha \mapsto -1-\alpha }$.

The exceptional Lie superalgebra ${\displaystyle F($4)} .

It has dimension (24|16). Its even part is given by ${\displaystyle {\mathfrak {sl}}($2)\oplus {\mathfrak {so}}(7)} .

The exceptional Lie superalgebra ${\displaystyle G($3)} .

It has dimension (17|14). Its even part is given by ${\displaystyle {\mathfrak {sl}}($2)\oplus G_{2}} .

There are also two so-called strange series called ${\displaystyle {\mathfrak {pe}}($n)} and ${\displaystyle {\mathfrak {q}}($n)} .

The Cartan types. They can be divided in four families: ${\displaystyle W($n)} , ${\displaystyle S($n)} , ${\displaystyle {\widetilde {S}}(2n)}$ and ${\displaystyle H($n)} . For the Cartan type of simple Lie superalgebras, the odd part is no longer completely reducible under the action of the even part.

The classification consists of the 10 series W(m, n), S(m, n) ((m, n) ≠ (1, 1)), H(2m, n), K(2m + 1, n), HO(m, m) (m ≥ 2), SHO(m, m) (m ≥ 3), KO(m, m + 1), SKO(m, m + 1; β) (m ≥ 2), SHO ~ (2m, 2m), SKO ~ (2m + 1, 2m + 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 superstring theory. Specifically, the Virasoro algebras with ${\displaystyle {\mathcal {N}}}$ supersymmetries are ${\displaystyle K(1,{\mathcal {N}})}$ which only have central extensions up to ${\displaystyle {\mathcal {N}}=4}$.^[7]

Incategory theory, a Lie superalgebra can be defined as a nonassociative superalgebra whose product satisfies

• ${\displaystyle [\cdot ,\cdot ]\circ ({\operatorname {id} }+\tau _{A,A})=0}$
• ${\displaystyle [\cdot ,\cdot ]\circ ([\cdot ,\cdot ]\otimes {\operatorname {id} }\circ ({\operatorname {id} }+\sigma +\sigma ^{2})=0}$

where σ is the cyclic permutation braiding ${\displaystyle ({\operatorname {id} }\otimes \tau _{A,A})\circ (\tau _{A,A}\otimes {\operatorname {id} })}$. In diagrammatic form:

• Gerstenhaber algebra
• Anyonic Lie algebra
• Grassmann algebra
• Representation of a Lie superalgebra
• Superspace
• Supergroup
• Universal enveloping algebra

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• Irving Kaplansky + Lie Superalgebras