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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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Published in: | Lobachevskii journal of mathematics 2017-03, Vol.38 (2), p.255-261 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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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. |
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ISSN: | 1995-0802 1818-9962 |
DOI: | 10.1134/S199508021702007X |