- Vertex operator algebra
In
mathematics , a vertex operator algebra (VOA) is an algebraic structure that plays an important role inconformal field theory and related areas of physics. They have proven useful in purely mathematical contexts such asmonstrous moonshine and thegeometric Langlands correspondence .Vertex operator algebras were first introduced by
Richard Borcherds in1986 , motivated by the vertex operators arising from field insertions in two dimensional conformal field theory. Important examples include lattice VOAs (modeling lattice CFTs), VOAs given by representations of affine Kac-Moody algebras (from the WZW model), the Virasoro VOAs (i.e., VOAs corresponding to representations of theVirasoro algebra ) and themoonshine module "V"♮, constructed by Frenkel, Lepowsky and Meurman in1988 . The axioms of a vertex operator algebra are a formal algebraic interpretation of what physicists calledchiral algebra s, whose definition was made mathematically rigorous byAlexander Beilinson andVladimir Drinfel'd .Motivation
The axioms of a vertex algebra are obtained from abstracting away the essentials of the
operator product expansion of operators in a 2D Euclideanchiral conformal field theory . The two dimensional Euclidean space is treated as aRiemann sphere with a point added at infinity. V is taken to be the space of all operators at . The operator product expansion is holomorphic in z and so, we can make aLaurent expansion of it. 1 is the identity operator. We treat an operator valued holomorphic map over as aformal Laurent series . This is denoted by the notation V((z)). A holomorphic map over is given by aTaylor series and as aformal power series , this is denoted byV .z The operator b(0) is abstracted to b and the operator a(z) to Y(a,z). The derivative a'(z) is abstracted to -Ta.
Formal definition
A vertex algebra is a vector space "V", together with an identity element 1 , an
endomorphism "T", and a multiplication map:
written:
:
satisfying the following axioms:
- (Identity) For any "a" ∈ "V",
: and
- (Translation) "T(1) = 0", and for any "a", "b" ∈ "V",
:
- (Four point function) For any "a", "b", "c" ∈ "V", there is an element
:
such that "Y(a,z)Y(b,w)c", "Y(b,w)Y(a,z)c", and "Y(Y(a,z-w)b,w)c" are the expansions of "X(a,b,c;z,w)" in "V((z))((w))", "V((w))((z))", and "V((w))((z-w))", respectively.
The multiplication map is often written as a state-field correspondence
:
associating an operator-valued formal distribution (called a vertex operator) to each vector. Physically, the correspondence is an insertion at the origin, and "T" is a generator of infinitesimal translations. The four-point axiom combines associativity and commutativity, up to singularities. Note that the translation axiom implies "Ta = a"-2"1", so "T" is determined by "Y".
A vertex algebra"V" is Z+-graded if
:
such that if "a" ∈ Vk and "b" ∈ Vm, then "a"n "b" ∈ Vk+m-n-1.
A vertex operator algebra is a Z+-graded vertex algebra equipped with a Virasoro element ω ∈ "V"2, such that the vertex operator
:
satisfies for any "a" ∈ "V"n, the relations:
References
* Richard Borcherds, "Vertex algebras, Kac-Moody algebras, and the Monster", "Proc. Natl. Acad. Sci. USA." 83 (1986) 3068-3071
* Igor Frenkel, James Lepowsky, Arne Meurman, "Vertex operator algebras and the Monster". "Pure and Applied Mathematics, 134." Academic Press, Inc., Boston, MA, 1988. liv+508 pp. ISBN 0-12-267065-5
*Victor Kac , "Vertex algebras for beginners". "University Lecture Series, 10." American Mathematical Society, 1998. viii+141 pp. ISBN 0-8218-0634-2
* Edward Frenkel, David Ben-Zvi, "Vertex algebras and Algebraic Curves". "Mathematical Surveys and Monographs, 88." American Mathematical Society, 2001. xii+348 pp. ISBN 0-8218-2894-0- (Identity) For any "a" ∈ "V",
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