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To a correlation function in a two-dimensional conformal field theory with the central charge $c=1$, we associate a matrix differential equation $\Psi' = L \Psi$, where the Lax matrix $L$ is a matrix square root of the energy-momentum tensor.
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A. B. Zamolodchikov, A. B. Zamolodchikov (1996) Structure constants and conformal bootstrap in Liouville field theory
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I. Runkel, G. M. T. Watts (2001) A non-rational CFT with c = 1 as a limit of minimal models
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V. Schomerus (2003) Rolling tachyons from Liouville theory
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A. Bytsko, J. Teschner (2009) The integrable structure of nonrational conformal field theory
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M. Bergere, B. Eynard (2009) Determinantal formulae and loop equations
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O. Gamayun, N. Iorgov, O. Lisovyy (2012) Conformal field theory of Painlevé VI
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