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The Lie algebra $so(2n+1)$ and the Lie superalgebra $osp(1/2n)$ are quantized in terms of $3n$ generators, called preoscillator generators. Apart from $n$ "Cartan" elements the preoscillator generators are deformed para-Fermi operators in…

High Energy Physics - Theory · Physics 2011-04-15 Tchavdar D. Palev

We have examined the deformation of a generic non-Abelian gauge theory obtained by replacing its Lie group by the corresponding quantum group. This deformed gauge theory has more degrees of freedom than the theory from which it is derived.…

High Energy Physics - Theory · Physics 2009-11-07 R. J. Finkelstein

A deformation of the harmonic oscillator algebra associated with the Morse potential and the SU(2) algebra is derived using the quantum analogue of the anharmonic oscillator. We use the quantum oscillator algebra or $q$-boson algebra which…

Statistical Mechanics · Physics 2011-12-20 Maia Angelova , V. K. Dobrev , A. Frank

Mean field theory has an unexpected group theoretic mathematical foundation. Instead of representation theory which applies to most group theoretic quantum models, Hartree-Fock and Hartree-Fock-Bogoliubov have been formulated in terms of…

Nuclear Theory · Physics 2007-05-23 Ts. Dankova , G. Rosensteel

We analyze among all possible quantum deformations of the 3+1 (anti)de Sitter algebras, so(3,2) and so(4,1), which have two specific non-deformed or primitive commuting operators: the time translation/energy generator and a rotation. We…

High Energy Physics - Theory · Physics 2014-11-18 Angel Ballesteros , N. Rossano Bruno , Francisco J. Herranz

A two-parameter deformed superoscillator system with SUq1/q2(n|m)-covariance is presented and used to construct a two-parameter deformed N=2 SUSY algebra. The Fock space representation of the algebra is discussed and the deformed…

High Energy Physics - Theory · Physics 2011-07-28 Abdullah Algin , Metin Arik , Ali Serdar Arikan

Within the standard quantum mechanics a q-deformation of the simplest N=2 supersymmetry algebra is suggested. Resulting physical systems do not have conserved charges and degeneracies in the spectra. Instead, superpartner Hamiltonians are…

High Energy Physics - Theory · Physics 2015-06-26 V. Spiridonov

Starting with a Hilbert space endowed with a representation of a unitary Lie algebra and an action of a generalized Dirac operator, we develop a mathematical concept towards gauge field theories. This concept shares common features with the…

High Energy Physics - Theory · Physics 2008-02-03 Raimar Wulkenhaar

The non-standard quantum deformation of the (trivially) extended sl(2,R) algebra is used to construct a new quantum deformation of the two-photon algebra h_6 and its associated quantum universal R-matrix. A deformed one-boson representation…

q-alg · Mathematics 2009-10-30 Angel Ballesteros , Francisco J. Herranz , Preeti Parashar

A Poisson coalgebra analogue of a (non-standard) quantum deformation of sl(2) is shown to generate an integrable geodesic dynamics on certain 2D spaces of non-constant curvature. Such a curvature depends on the quantum deformation parameter…

High Energy Physics - Theory · Physics 2009-11-11 Angel Ballesteros , Francisco J. Herranz , Orlando Ragnisco

An abstract Newton-like equation on a general Lie algebra is introduced such that orbits of the Lie-group action are attracting set. This equation generates the nonlinear dynamical system satisfied by the group parameters having an…

chao-dyn · Physics 2007-05-23 K. Kowalski , J. Rembielinski

Applications of algebras in physics are related to the connection of measurable observables to relevant elements of the algebras, usually the generators. However, in the determination of the generators in Lie algebras there is place for…

Quantum Algebra · Mathematics 2009-11-13 A. Ballesteros , E. Celeghini , M. A. del Olmo

The Lie algebra $\mathfrak{su}(1,1)$ can be deformed by a reflection operator, in such a way that the positive discrete series representations of $\mathfrak{su}(1,1)$ can be extended to representations of this deformed algebra…

Mathematical Physics · Physics 2012-05-14 Elchin I. Jafarov , Neli I. Stoilova , Joris Van der Jeugt

This paper shows how to construct classical and quantum field C*-algebras modeling a $U(1)^n$-gauge theory in any dimension using a novel approach to lattice gauge theory, while simultaneously constructing a strict deformation quantization…

Mathematical Physics · Physics 2022-04-20 T. D. H. van Nuland

We propose a new structure ${\cal U}^{r}_{\displaystyle{q}}(sl(2)) $. This is realized by multiplying $\delta$ ($q=e^{\delta}$, $\delta\in \CC$) by $\theta$, where $\theta$ is a real nilpotent -paragrassmannian- variable of order $r$…

q-alg · Mathematics 2009-10-28 B. Abdesselam , J. Beckers , A. Chakrabarti , N. Debergh

Multiparametric quantum deformations of $gl(2)$ are studied through a complete classification of $gl(2)$ Lie bialgebra structures. From them, the non-relativistic limit leading to harmonic oscillator Lie bialgebras is implemented by means…

Quantum Algebra · Mathematics 2009-10-31 Angel Ballesteros , Francisco J. Herranz , Preeti Parashar

We derive the master function governing the component action of the four-dimensional non-anticommutative (NAC) and fully N=2 supersymmetric gauge field theory with a non-simple gauge group U(2)=SU(2)xU(1). We use a Lorentz singlet…

High Energy Physics - Theory · Physics 2016-09-06 Sergei V. Ketov , Shin Sasaki

We consider the symmetry algebra generated by the total angular momentum operators, appearing as constants of motion of the $\mathrm{S}_3$ Dunkl Dirac equation. The latter is a deformation of the Dirac equation by means of Dunkl operators,…

Mathematical Physics · Physics 2018-01-11 Hendrik De Bie , Roy Oste , Joris Van der Jeugt

We develop here a simple formalism that converts the second-class constraints into first-class ones for a particle moving on the $n$-dimensional sphere. The Poisson algebra generated by the Hamiltonian and the constraints closes and by…

High Energy Physics - Theory · Physics 2007-05-23 Petre Diţă

The spectrum of the square of the angular momentum in arbitrary dimensions is derived using only group theoretical techniques. This is accomplished by application of the Lie algebra of the noncompact group O(2,1).

Mathematical Physics · Physics 2012-11-15 Tamar Friedmann , C. R. Hagen