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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.
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