Towards new relativistic doubly $\kappa$-deformed D=4 quantum phase spaces

Abstract

We propose new noncommutative models of quantum phase spaces, containing a pair of $\kappa$-deformed Poincaré algebras, with two independent double ($\kappa ,\tilde{\kappa }$)-deformations in space-time and four-momenta sectors. The first such quantum phase space can be obtained by contractions $M,R\to \infty$ of recently introduced doubly $\kappa$-deformed $(\kappa ,\tilde{\kappa })$-Yang models, with the parameters $M,R$ describing inverse space-time and four-momenta curvatures and constant four-vectors $a_{\mu },b_{\mu }$ determining nine types of $(\kappa ,\tilde{\kappa })$-deformations. The second considered model is provided by the nonlinear doubly $\kappa$-deformed TSR algebra spanned by 14 coset $\hat{o}(1,5)/\hat{o}(2)$ generators. The basic algebraic difference between the two models is the following: the first one, described by $\hat{o}(1,5)$ Lie algebra can be supplemented by the Hopf algebra structure, while the second model contains the quantum phase space commutators $[{\hat{x}}_{\mu },{\hat{q}}_{\nu }]$, with the standard numerical $i\hslash {\eta }_{\mu \nu }$ term; therefore it describes the quantum-deformed Heisenberg algebra relations which cannot be equipped with the Hopf algebra.

arXiv comment13 pages, extended version, one section added, reference list expanded, published version

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Cited by in corpus (1)

• Symplectic realization of generalized Snyder-Poisson algebra