sigma07-026. 320KB Jun 04 2011 12:10:00 AM
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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
The study of possible generalizations to Finsler manifolds should be seen as a first step towards further generalizations to arbitrary metric tensor fields along the tangent
In higher dimensions, the usual highest weight representations apply for the symmetry algebra of the Laplace–Beltrami operator. In this case there is no longer a single chain
In more detail the structure of the paper is as follows: In next section we describe shortly two one-dimensional classical systems which can be considered as generalizations of
In particular, it has been shown that their integrals of motion generate a quadratic Poisson algebra (in the classical case) or a quadratic associative algebra (in the quantum one)
applying the Gessel–Viennot path method with an additional involution and a deformation of paths, we obtain an expression by a positive sum over a set of tuples of paths, which
Quantization method for the Friedmann–Lemaˆıtre Universe based on the canonical Hamilton equations of motion is proposed and quantum information theory way to physics of the Universe
We investigate spectral properties of a quantum particle confined to an infinite straight planar strip by imposing Robin boundary conditions with variable coupling.. As- suming that
