Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
1843527 | Nuclear Physics B | 2006 | 28 Pages |
Abstract
The M(3,p) minimal models are reconsidered from the point of view of the extended algebra whose generators are the energy-momentum tensor and the primary field Ï2,1 of dimension (pâ2)/4. Within this framework, we provide a quasi-particle description of these models, in which all states are expressed solely in terms of the Ï2,1-modes. More precisely, we show that all the states can be written in terms of Ï2,1-type highest-weight states and their Ï2,1-descendants. We further demonstrate that the conformal dimension of these highest-weight states can be calculated from the Ï2,1 commutation relations, the highest-weight conditions and associativity. For the simplest models (p=5,7), the full spectrum is explicitly reconstructed along these lines. For p odd, the commutation relations between the Ï2,1 modes take the form of infinite sums, i.e., of generalized commutation relations akin to parafermionic models. In that case, an unexpected operator, generalizing the Witten index, is unraveled in the OPE of Ï2,1 with itself. A quasi-particle basis formulated in terms of the sole Ï2,1 modes is studied for all allowed values of p. We argue that it is governed by jagged-type partitions further subject a difference 2 condition at distance 2. We demonstrate the correctness of this basis by constructing its generating function, from which the proper fermionic expression of the combination of the Virasoro irreducible characters Ï1,s and Ï1,pâs (for 1⩽s⩽[p/3]+1) are recovered. As an aside, a practical technique for implementing associativity at the level of mode computations is presented, together with a general discussion of the relation between associativity and the Jacobi identities.
Related Topics
Physical Sciences and Engineering
Mathematics
Mathematical Physics
Authors
P. Jacob, P. Mathieu,