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A theorem on generalized nonions and their properties for the applied structures in physics

The central part of the paper consists of a theorem on generalized nonions governing dynamical systems modelling of special ternary, quaternary, quinary, senary, etc. structures, due to the third named author. Let M n (C), n ≥ 2, be the set of n × n -matrices with complex entries. The theorem states...

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Bibliographic Details
Published in:Lobachevskii journal of mathematics 2017-03, Vol.38 (2), p.255-261
Main Authors: Frątczak, E. Z., Ławrynowicz, J., Nowak-Kępczyk, M., Polatoglou, H. M., Wojtczak, L.
Format: Article
Language:English
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Summary:The central part of the paper consists of a theorem on generalized nonions governing dynamical systems modelling of special ternary, quaternary, quinary, senary, etc. structures, due to the third named author. Let M n (C), n ≥ 2, be the set of n × n -matrices with complex entries. The theorem states that in M n (C) there exists a basis such that PQ − λ s QP = 0, s = 0, 1, 2,.., n − 1, where { P,Q ,}, u , v are specified in Section 1, formulae (1) and (2).The particular cases n = 2, 3, 4 with other choices of u , v were discussed by James Joseph Sylvester (1883, 1884) and by Charles Sanders Peirce (1882).In particular, λ = j, j 3 = 1, j ≠ 1, generates nonions. Before the section on the above theorem and its visualization on a two-sheeted Riemann surface, we give three physical motivations for the topic: controlled noncommutativity: Sylvester–Peirce approach vs. Max Planck approach (1900), supersonic flow of a ternary alloy in gas, and changing hexagonal to pentagonal structure in pentacene.
ISSN:1995-0802
1818-9962
DOI:10.1134/S199508021702007X