sigma06-066. 280KB Jun 04 2011 12:09:54 AM
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![Table 4. Addition and multiplication in R⊥ (top) and in GF(4) ≃ GF(2)[x]/⟨x2 + x + 1⟩ (bottom).](https://thumb-ap.123doks.com/thumbv2/123dok/1158363.899291/8.612.119.501.80.228/table-addition-multiplication-r-gf-gf-x-x.webp)
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In this contribution we applied the iterative procedure of obtaining the eigenvectors for quantum integrable systems by Kharchev and Lebedev [ 7 ] (which has origin in [ 8 ]
Key words: anomalously slow cross symmetry phase relaxation; Bi( γ ,p) photonuclear com- pound reaction; quantum chaos; thermalized non-equilibrated matter; quantum computing..
It was shown that, for all examples of invariant differential equations from the Lie’s list, there ex- ist non-point linearizing transformations (which transform the family of
In the last four decades, much attention has been paid to the problem of describing processes of interaction of charged matter with electromagnetic radiation at resonance [ 1 , 2 , 3
Our approach is built on making gauge copies of an extended AKNS model labeled by angle θ belonging to an interval 0 ≤ θ ≤ π/ 2 and then by elimination of one of two components of
Department of Mathematical Sciences, University of Wisconsin-Milwaukee, P. Classical ellipsoidal and sphero-conal harmonics are polynomial solutions of the Laplace equation that can
Abstract. We define the coupled modified KP hierarchy and its dispersionless limit. This integrable hierarchy is a generalization of the “half” of the Toda lattice hierarchy as well
This divergence is exactly the same which is found in the perturbative calculation for the quantum theory defined in the Groenewold–Moyal plane [ 22 ], therefore in this case
