2001
DOI: 10.1006/aphy.2001.6159
|View full text |Cite
|
Sign up to set email alerts
|

Generalized Lorentz-Force Equations

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
14
0

Year Published

2003
2003
2016
2016

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 18 publications
(14 citation statements)
references
References 17 publications
0
14
0
Order By: Relevance
“…The polynomial r (Y ) is called the invariant polynomial [11] . By applying Y = X − P 1 /n for every root we get…”
Section: Applications Of the Pascal Matrix Transformation Reduction Omentioning
confidence: 99%
“…The polynomial r (Y ) is called the invariant polynomial [11] . By applying Y = X − P 1 /n for every root we get…”
Section: Applications Of the Pascal Matrix Transformation Reduction Omentioning
confidence: 99%
“…Indeed, these two fundamental features allow for deriving many aspects of the canonical statistical mechanical formalism without recourse to the detailed structure of standard Hamiltonian dynamics [24,25]. Among others, the Lotka-Volterra predator-prey systems [26,27] and the Nambu systems [28][29][30][31][32][33] share the vanishing divergence property and admit an integral of motion. If the system A is to behave as a proper "information storage device", it is reasonable to assume that before and after the information erasure process, the systems A and B are only weakly coupled.…”
Section: Divergenceless Dynamical Systemsmentioning
confidence: 99%
“…The Nambu dynamical structures arise in a natural way in several contexts. For instance, Nambu dynamics has been applied to the relativistic dynamics of charged spinning particles [32], and to some hydrodynamical type systems [33].…”
mentioning
confidence: 99%
“…In this section we will consider a simplified Nambu system based on a three dimensional phase space coordinatised by the triplet {x, p, q} within the following physical interpretation [16,17,18]: we take the physical system as formed by a real (corporeal) particle of mass m which is localised in a given point by the coordinates (x, P ) of two dimensional phase space, hence the position of the real particle is given by the coordinate x while its momentum is given by the coordinate P . This system will be considered as a composed system, formed by two subparticles with momenta p and q, and masses m p and m q , respectively; this situation is directly generalised to three dimensional triplet configuration space ( x, p, q).…”
Section: Relativistic Yamaleev's Frameworkmentioning
confidence: 99%
“…However, first attempts to understand the kind of mechanics involved within such formalism were not fruitful leaving the question to the exploration of some similarities and interrelations between Hamiltonian formalism and Newton mechanics. It is only by considering Yamaleev's construction that we obtain a complete realisation of Nambu formalism into real mechanics [16,17,18].…”
Section: Introductionmentioning
confidence: 99%