2010
DOI: 10.1063/1.3460841
|View full text |Cite
|
Sign up to set email alerts
|

Possible quantum kinematics. II. Nonminimal case

Abstract: The quantum analogs of the N-dimensional Cayley-Klein spaces with different combinations of quantum and Cayley-Klein structures are described for non-minimal multipliers, which include the first and the second powers of contraction parameters in the transformation of deformation parameter. The noncommutative analogs of (N − 1)-dimensional constant curvature spaces are introduced. Part of these spaces for N = 5 are interpreted as the noncommutative analogs of (1 + 3) space-time models. As a result the wide vari… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
6
0

Year Published

2013
2013
2022
2022

Publication Types

Select...
4
2
1

Relationship

0
7

Authors

Journals

citations
Cited by 8 publications
(6 citation statements)
references
References 12 publications
(15 reference statements)
0
6
0
Order By: Relevance
“…A more challenging situation occurs if we have a degenerate metric and cycles are represented by parabolas [32] and respective FLT are based on dual numbers [4]. Besides theoretical interest such spaces are meaningful physical models [14,15,32]. The differential geometry loses its ground in the degenerate case and non-commutative/non-local effects appear [20, § 7.2].…”
Section: Discussion and Generalisationsmentioning
confidence: 99%
See 2 more Smart Citations
“…A more challenging situation occurs if we have a degenerate metric and cycles are represented by parabolas [32] and respective FLT are based on dual numbers [4]. Besides theoretical interest such spaces are meaningful physical models [14,15,32]. The differential geometry loses its ground in the degenerate case and non-commutative/non-local effects appear [20, § 7.2].…”
Section: Discussion and Generalisationsmentioning
confidence: 99%
“…The differential geometry loses its ground in the degenerate case and non-commutative/non-local effects appear [20, § 7.2]. The presence of zero divisors among dual numbers prompts a projective approach [5; 20, § 4.5] to the cross ratio of four dual numbers, which replaces (14). Variational methods do not produce FLT-invariant family of geodesics in the degenerate case, instead geometry of cycles need to be employed [18].…”
Section: Discussion and Generalisationsmentioning
confidence: 99%
See 1 more Smart Citation
“…It is common [15], [13], [55], [30], [29] to consider mainly Clifford algebras Cℓ(n, =)Cℓ(n, 0, 0,) of the Euclidean space or the algebra Cℓ(p, q, =)Cℓ(p, q, 0,) of the pseudo-Euclidean (Minkowski) spaces. However, Clifford algebras Cℓ(p, q, r,), r > 0 with nilpotent generators e 2 i = 0 correspond to interesting geometry [41], [35], [61], [52] and physics [25], [23], [24], [42], [43], [47] as well. Yet, the geometry with idempotent units in spaces with dimensionality n > 2 is still not sufficiently elaborated.…”
Section: Möbius-lie Geometry and The Cycle Librarymentioning
confidence: 99%
“…The family P τ,t consists of the eigenvectors of the 4 × 4 matrix from (28) with suitably substituted entries. There is (up to a factor) exactly one τ -isotropic form in P τ,t , namely 1 τ 1 1 .…”
Section: 4mentioning
confidence: 99%