Hidden Grassmann Structure in the XXZ Model II: Creation Operators

被引:84
作者
Boos, H. [1 ]
Jimbo, M. [2 ,3 ]
Miwa, T. [4 ]
Smirnov, F. [5 ]
Takeyama, Y. [6 ]
机构
[1] Univ Wuppertal, Dept Phys, D-42097 Wuppertal, Germany
[2] Univ Tokyo, Grad Sch Math Sci, Tokyo 1538914, Japan
[3] Inst Phys & Math Universe, Chiba 2778582, Japan
[4] Kyoto Univ, Grad Sch Sci, Dept Math, Kyoto 6068502, Japan
[5] Univ Paris 06, Phys Theor & Hautes Energies Lab, F-75252 Paris 05, France
[6] Univ Tsukuba, Dept Math, Grad Sch Pure & Appl Sci, Tsukuba, Ibaraki 3058571, Japan
关键词
FIELD;
D O I
10.1007/s00220-008-0617-z
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
In this article we unveil a new structure in the space of operators of the XXZ chain. For each a we consider the space W-alpha of all quasi-local operators, which are products of the disorder field q(alpha Sigma jo=-infinity sigma j3) with arbitrary local operators. In analogy with CFT the disorder operator itself is considered as primary field. In our previous paper, we have introduced the annhilation operators b(zeta), c(zeta) which mutually anti-commute and kill the "primary field". Here we construct the creation counterpart b*(zeta), c*(zeta) and prove the canonical anti-commutation relations with the annihilation operators. We conjecture that the creation operators mutually anti-commute, thereby upgrading the Grassmann structure to the fermionic structure. The bosonic operator t*(zeta) is the generating function of the adjoint action by local integrals of motion, and commutes entirely with the fermionic creation and annihilation operators. Operators b*(zeta), c*(zeta), t*(zeta) create quasi-local operators starting from the primary field. We show that the ground state averages of quasi-local operators created in this way are given by determinants.
引用
收藏
页码:875 / 932
页数:58
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