Virasoro Algebra - Representation Theory

Representation Theory

A lowest weight representation of the Virasoro algebra is a representation generated by a vector that is killed by for, and is an eigenvector of and . The letters and are usually used for the eigenvalues of and on . (The same letter is used for both the element of the Virasoro algebra and its eigenvalue.) For every pair of complex numbers and there is a unique irreducible lowest weight representation with these eigenvalues.

A lowest weight representation is called unitary if it has a positive definite inner product such that the adjoint of is . The irreducible lowest weight representation with eigenvalues h and c is unitary if and only if either c≥1 and h≥0, or c is one of the values

for m = 2, 3, 4, .... and h is one of the values

for r = 1, 2, 3, ..., m−1 and s= 1, 2, 3, ..., r. Daniel Friedan, Zongan Qiu, and Stephen Shenker (1984) showed that these conditions are necessary, and Peter Goddard, Adrian Kent and David Olive (1986) used the coset construction or GKO construction (identifying unitary representations of the Virasoro algebra within tensor products of unitary representations of affine Kac-Moody algebras) to show that they are sufficient. The unitary irreducible lowest weight representations with c < 1 are called the discrete series representations of the Virasoro algebra. These are special cases of the representations with m = q/(pq), 0<r<q, 0< s<p for p and q coprime integers and r and s integers, called the minimal models and first studied in Belavin et al. (1984).

The first few discrete series representations are given by:

  • m = 2: c = 0, h = 0. The trivial representation.
  • m = 3: c = 1/2, h = 0, 1/16, 1/2. These 3 representations are related to the Ising model
  • m = 4: c = 7/10. h = 0, 3/80, 1/10, 7/16, 3/5, 3/2. These 6 representations are related to the tri critical Ising model.
  • m = 5: c = 4/5. There are 10 representations, which are related to the 3-state Potts model.
  • m = 6: c = 6/7. There are 15 representations, which are related to the tri critical 3-state Potts model.

The lowest weight representations that are not irreducible can be read off from the Kac determinant formula, which states that the determinant of the invariant inner product on the degree h+N piece of the lowest weight module with eigenvalues c and h is given by

which was stated by V. Kac (1978), (see also Kac and Raina 1987) and whose first published proof was given by Feigin and Fuks (1984). (The function p(N) is the partition function, and AN is some constant.) The reducible highest weight representations are the representations with h and c given in terms of m, c, and h by the formulas above, except that m is not restricted to be an integer ≥ 2 and may be any number other than 0 and 1, and r and s may be any positive integers. This result was used by Feigin and Fuks to find the characters of all irreducible lowest weight representations.

Read more about this topic:  Virasoro Algebra

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