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Logarithmic conformal field theory : ウィキペディア英語版
Logarithmic conformal field theory
In theoretical physics, a logarithmic conformal field theory is a generalization of the concept of (usually two-dimensional) conformal field theory in which the correlators of the basic fields are allowed to be multi-valued and functions of the logarithm of the separation of the operators.
==References==

(Logarithmic conformal field theory on arxiv.org )
* V. Gurarie, (''Logarithmic operators in conformal field theory'' ), Nucl. Phys. B410 (1993) 535-549.
* M. R. Gaberdiel, H. G. Kausch, ("Indecomposable fusion products" ), Nucl. Phys. B477 (1996) 293-318.
* M. Reza Rahimi Tabar, A. Aghamohammadi and M. Khorrami, ''The logarithmic conformal field theories'', Nucl. Phys. B497 (1997) 555-566.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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