sigma06-078. 224KB Jun 04 2011 12:09:55 AM
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The operator gauge invariant Maxwell’s equations and corresponding charge conservation are obtained by defining the generalized derivatives of the f irst and
As it was demonstrated recently, the approach first proposed in [13, 14] based on some set of q - deformed oscillators along with the related model of ideal gas of q -bosons is
We prove that the relevant B¨acklund transformation preserves the reality of the n -soliton potentials and establish their pole structure with respect to the broadening parameter..
[16] Atoyan A., Patera J., Properties of continuous Fourier extension of the discrete cosine transform and its multidimensional generalization, J. [21] Humphreys J., Introduction to
Due to Theorem 1 the Killing vector fields which we obtain by {K , K} are parallel with respect to the Levi-Civita connection if K is strongly torsion
For that, we take an inspiration from the case u = 0 where the sum of the left and right currents can be interpreted as the product in the Abelian cosymmetry group L K (the
We use this result and the formula of Le and Murakami for the Knizhnik–Zamolodchikov (KZ) associator Φ to derive a formula for log(Φ) in terms of MZV’s (multiple zeta values)..
The Taub-NUT space has a special geometry where the covariantly constant K-Y tensors exist by virtue of the metric being self-dual and the Dirac-type operators generated by them
