2008/10/31 by Yas-Hiro Quano
Mathematics · Physics and Astronomy · #Advanced Algebra and Geometry #Algebraic structures and combinatorial models #Quantum and Classical Electrodynamics #hep-th #math.QA
paper · pdf · doi:10.1088/1751-8113/42/16/165211
published as J. Phys. A: Math. Theor. 42 (2009) 165211, 20pages · For the next thirty days the full text of this article is available at http://stacks.iop.org/1751-8121/42/165211
openalex publication_date 2009/04/01 · arxiv created 2009/04/02 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/30
Belavin's ( / n )-symmetric model is considered on the basis of bosonization of vertex operators in the A (1) n −1 model and vertex–face transformation. The corner transfer matrix (CTM) Hamiltonian of the ( / n )-symmetric model and tail operators are expressed in terms of bosonized vertex operators in the A (1) n −1 model. Correlation functions of the ( / n )-symmetric model can be obtained by using these objects, in principle. In particular, we calculate spontaneous polarization, which reproduces the result we obtained in 1993.