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In Theorem 4 below we prove that the space of shifted singular polynomials is isomorphic to that of singular polynomials as C S n -modules, and it has a basis consisting of
As a first step towards a geometric construction of asymptotic expansions for the Moyal type restriction, we obtain an integral representation for the Moyal restriction
In particular we conclude that the Lorentz covariant nonlinear Dirac equations we have explicitly studied in this paper are not gauge equivalent to the linear Dirac equation.
In this paper we compute matrix elements for the composition of the type I intertwining operators [5] associated to finite dimensional irreducible representations of U q ( sl 2 )..
It is known, that the moduli space of flat bundles are deformation (the Whitham deformation) of the phase spaces of the Hitchin integrable systems – the moduli spaces of the
In Section 3 we use this set up to prove Theorem 3.1 , which characterizes the boundaries of graphs of harmonic functions using the moment conditions arising from conservation laws..
Key words: homogeneous spaces, weakly symmetric spaces, homogeneous spaces of posi- tive Euler characteristic, geodesic orbit spaces, normal homogeneous Riemannian
We study in Section 4 the Dunkl convolution product and the Dunkl transform of distributions which will be useful in the sequel, and when the multiplicity function takes integer
