Abstract:In the past ten years, the ideas of supersymmetry have been profitably applied to many nonrelativistic quantum mechanical problems. In particular, there is now a much deeper understanding of why certain potentials are analytically solvable and an array of powerful new approximation methods for handling potentials which are not exactly solvable. In this report, we review the theoretical formulation of supersymmetric quantum mechanics and discuss many applications. Exactly solvable potentials can be understood i… Show more
“…To close this section, let us mention that the k-fermions introduced in [9,10] share some common properties with the parafermions of order k − 1 discussed in [35,36,37,38,39,40,41]. Indeed, a parafermionic algebra of order k−1 corresponds to a fractional supersymmetric algebra of order k.…”
Abstract. This paper deals with quon algebras or deformed oscillator algebras, for which the deformation parameter is a root of unity. We motivate why such algebras are interesting for fractional supersymmetric quantum mechanics, angular momentum theory and quantum information. More precisely, quon algebras are used for (i) a realization of a generalized Weyl-Heisenberg algebra from which it is possible to associate a fractional supersymmetric dynamical system, (ii) a polar decomposition of SU 2 and (iii) a construction of mutually unbiased bases in Hilbert spaces of prime dimension. We also briefly discuss (symmetric informationally complete) positive operator valued measures in the spirit of (iii).
“…To close this section, let us mention that the k-fermions introduced in [9,10] share some common properties with the parafermions of order k − 1 discussed in [35,36,37,38,39,40,41]. Indeed, a parafermionic algebra of order k−1 corresponds to a fractional supersymmetric algebra of order k.…”
Abstract. This paper deals with quon algebras or deformed oscillator algebras, for which the deformation parameter is a root of unity. We motivate why such algebras are interesting for fractional supersymmetric quantum mechanics, angular momentum theory and quantum information. More precisely, quon algebras are used for (i) a realization of a generalized Weyl-Heisenberg algebra from which it is possible to associate a fractional supersymmetric dynamical system, (ii) a polar decomposition of SU 2 and (iii) a construction of mutually unbiased bases in Hilbert spaces of prime dimension. We also briefly discuss (symmetric informationally complete) positive operator valued measures in the spirit of (iii).
“…These equations are reminiscent of the defining equations for the parasupersymmetry of order p, [4]. In section 5, We shall use these equations to establish that every orthosupersymmetric system of order p has a parasupersymmetry of order p.…”
Section: The Ladder Operators Of the Canonical Representationmentioning
confidence: 99%
“…These equations indicate that the system has a parasupersymmetry [4] of order p generated by Q and a fractional supersymmetry [5] of order p + 1 generated by Q.…”
Section: An Orthosupersymmetric Realization Of Parasuper-mentioning
We construct a canonical irreducible representation for the orthofermion algebra of arbitrary order, and show that every representation decomposes into irreducible representations that are isomorphic to either the canonical representation or the trivial representation. We use these results to show that every orthosupersymmetric system of order p has a parasupersymmetry of order p and a fractional supersymmetry of order p + 1.
“…By combining both concepts within the framework of quantum mechanics, one gets variants of SSQM: paraSSQM [1,2,3], pseudoSSQM [4,5], and orthoSSQM [6].…”
Section: Introductionmentioning
confidence: 99%
“…For two particles, the S 2 -extended oscillator algebra A (2) κ , where S 2 = { I, K | K 2 = I }, is generated by the operators I, a † , a, N, K, subject to the Hermiticity conditions a † † = a, N † = N, K † = K −1 , and the relations…”
We consider the problem of bosonizing supersymmetric quantum mechanics (SSQM) and some of its variants, i.e., of realizing them in terms of only boson-like operators without fermion-like ones. In the SSQM case, this is realized in terms of the generators of the Calogero-Vasiliev algebra (also termed deformed Heisenberg algebra with reflection). In that of the SSQM variants, this is done by considering generalizations of the latter algebra, namely the C λ -extended oscillator algebras, where C λ is the cyclic group of order λ.
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