sigma10-077. 291KB Jun 04 2011 12:10:44 AM
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In the case N = 2, the nonlinear equations associated with the discrete Lax equation ( 27 ) are the same as in the 2-reduced A-case, i.e., those in Section 2 (as is to be expected
Section 3 contains the construction of the non-commutative punctured disk and the first type of noncommutative analogs of the operator from the previous section.. The operators here
are more or less two possible ways to construct the model: either one adds further terms in order to make the action gauge invariant (which will be discussed in the following
This paper was aimed to show how an interpretative procedure of divergent perturbative series, involving Mellin–Barnes representation and Borel resummation, leads to a
is compatible with the minimal canonical extension of the Doplicher–Fredenhagen–Roberts– Amorim (DFRA) algebra, is also invariant under an extended Poincar´e group of symmetry,
A representation of the affine Weyl groups can be lifted on the level of the τ functions [10, 11, 33], which gives rise to various bilinear equations of Hirota type satisfied the
We describe different versions of quantum Minkowski spacetime algebra; twisted equipped with h -adic topology and covariant with respect to quantized general linear group (Section 3
Molev gives a combinatorial formula for the Sklyanin determinant of twisted Yangians in terms of matrix elements of the matrix of generators of the twisted Yangians (see also [ 1