higgs algebra
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Author(s):  
A. N. Lavrenov ◽  
I. A. Lavrenov

In this paper, the q-generalization of the Higgs algebra is considered. The realization of this algebra is shown in an explicit form using a nonlinear transformation of the creation-annihilation operators of the q-harmonic oscillator. This transformation is the performance of two operations, namely, a “correction” using a function of the original Hamiltonian, and raising to the fourth power the creation and annihilation operators of a q-harmonic oscillator. The choice of the “correcting” function is justified by the standard form of commutation relations for the operators of the metaplectic realization Uq(SU(1,1)). Further possible directions of research are briefly discussed to summarize the results obtained. The first direction is quite obvious. It is the consideration of the problem when the dimension of the operator space increases or for any value N. The second direction can be associated with the analysis of the relationship between q-generalizations of the Higgs and Hahn algebras.


Author(s):  
А. N. Lavrenov ◽  
I. A. Lavrenov

In the light of the Howe duality, two different, but isomorphic representations of one algebra as Higgs algebra and Hahn algebra are considered in this article. The first algebra corresponds to the symmetry algebra of a harmonic oscillator on a 2-sphere and a polynomially deformed algebra SU(2), and the second algebra encodes the bispectral properties of corresponding homogeneous orthogonal polynomials and acts as a symmetry algebra for the Hartmann and certain ring-shaped potentials as well as the singular oscillator in two dimensions. The realization of this algebra is shown in explicit form, on the one hand, as the commutant O(4) ⊕ O(4) of subalgebra U(8) in the oscillator representation of universal algebra U (u(8)) and, on the other hand, as the embedding of the discrete version of the Hahn algebra in the double tensor product SU(1,1) ⊗ SU(1,1). These two realizations reflect the fact that SU(1,1) and U(8) form a dual pair in the state space of the harmonic oscillator in eight dimensions. The N-dimensional, N-fold tensor product SU(1,1)⊗N аnd q-generalizations are briefly discussed.


2018 ◽  
Vol 57 (7) ◽  
pp. 2133-2144
Author(s):  
T. Shreecharan ◽  
M. Naveen Kumar

2014 ◽  
Vol 29 (10) ◽  
pp. 1450050 ◽  
Author(s):  
Won Sang Chung

In this paper, Holstein–Primakoff realization of Higgs algebra is obtained by using the linear (or quadratic) deformation of Heisenberg algebra and q-deformed Higgs algebra is proposed. Some applications such as Kepler problem in a two-dimensional curved space and SUSY quantum mechanics are also discussed.


2003 ◽  
Vol 40 (1) ◽  
pp. 73-76 ◽  
Author(s):  
Ruan Dong ◽  
Wu Chu ◽  
Sun Hong-Zhou
Keyword(s):  

2000 ◽  
Vol 33 (22) ◽  
pp. 4073-4079 ◽  
Author(s):  
V V Gritsev ◽  
Yu A Kurochkin
Keyword(s):  

1999 ◽  
Vol 14 (17) ◽  
pp. 1149-1156 ◽  
Author(s):  
J. BECKERS ◽  
Y. BRIHAYE ◽  
N. DEBERGH

Supersymmetry in quantum optical models is pointed out here by dealing with differential realizations of the generators of the nonlinear Higgs algebra, when this algebra is seen as the spectrum generating algebra subtending the multi-boson Hamiltonians of such models.


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