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Conformally invariant elliptic Liouville equation and its symmetry preserving discretization

Abstract

The symmetry algebra of the real elliptic Liouville equation is an infinite-dimensional loop algebra with the simple Lie algebra o(3,1)o(3,1) as its maximal finite-dimensional subalgebra. The entire algebra generates the conformal group of the Euclidean plane E2E_2. This infinite-dimensional algebra distinguishes the elliptic Liouville equation from the hyperbolic one with its symmetry algebra that is the direct sum of two Virasoro algebras. Following a discretisation procedure developed earlier, we present a difference scheme that is invariant under the group O(3,1)O(3,1) and has the elliptic Liouville equation in polar coordinates as its continuous limit. The lattice is a solution of an equation invariant under O(3,1)O(3,1) and is itself invariant under a subgroup of O(3,1)O(3,1), namely the O(2)O(2) rotations of the Euclidean plane

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