N = 2 superconformal algebra


In mathematical physics, the 2D N = 2 superconformal algebra is an infinite-dimensional Lie superalgebra, related to supersymmetry, that occurs in string theory and two-dimensional conformal field theory. It has important applications in mirror symmetry. It was introduced by as a gauge algebra of the U fermionic string.

Definition

There are two slightly different ways to describe the N = 2 superconformal algebra, called the N = 2 Ramond algebra and the N = 2 Neveu–Schwarz algebra, which are isomorphic but differ in the choice of standard basis.
The N = 2 superconformal algebra is the Lie superalgebra with basis of even elements c, Ln, Jn, for n an integer, and odd elements G, G, where or defined by the following relations:
If in these relations, this yields the
N = 2 Ramond algebra; while if are
half-integers, it gives the N = 2 Neveu–Schwarz algebra. The operators generate a Lie subalgebra isomorphic to the Virasoro algebra. Together with the operators, they generate a Lie superalgebra isomorphic to the super Virasoro algebra,
giving the Ramond algebra if are integers and the Neveu–Schwarz algebra otherwise. When represented as operators on a complex inner product space, is taken to act as multiplication by a real scalar, denoted by the same letter and called the central charge, and the adjoint structure is as follows:

Properties

Free field construction

give a construction using two commuting real bosonic fields,
and a complex fermionic field
is defined to the sum of the Virasoro operators naturally associated with each of the three systems
where normal ordering has been used for bosons and fermions.
The current operator is defined by the standard construction from fermions
and the two supersymmetric operators by
This yields an N = 2 Neveu–Schwarz algebra with c = 3.

SU(2) supersymmetric coset construction

gave a coset construction of the N = 2 superconformal algebras, generalizing the coset constructions of for the discrete series representations of the Virasoro and super Virasoro algebra. Given a representation of the affine Kac–Moody algebra of SU at level with basis satisfying
the supersymmetric generators are defined by
This yields the N=2 superconformal algebra with
The algebra commutes with the bosonic operators
The space of physical states consists of eigenvectors of simultaneously annihilated by the 's for positive and the supercharge operator
The supercharge operator commutes with the action of the affine Weyl group and the physical states lie in a single orbit of this group, a fact which implies the Weyl-Kac character formula.

Kazama–Suzuki supersymmetric coset construction

generalized the SU coset construction to any pair consisting of a simple compact Lie group and a closed subgroup of maximal rank, i.e. containing a maximal torus of, with the additional condition that
the dimension of the centre of is non-zero. In this case the compact Hermitian symmetric space is a Kähler manifold, for example when. The physical states lie in a single orbit of the affine Weyl group, which again implies the Weyl–Kac character formula for the affine Kac–Moody algebra of.