2012
DOI: 10.1016/j.aop.2013.01.008
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A unified approach to quantum and classical TTW systems based on factorizations

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Cited by 29 publications
(66 citation statements)
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“…Examples of periodic and non-periodic orbits for this pasted potential are given in figure 2. For 'global' superintegrable systems all the bounded motions are periodic and the trajectories look like deformed Lissajous curves [10,11]. We should remark that such trajectories are smooth and they do not present 'angles' when crossing the boundary of a domain.…”
Section: (A) Superintegrable Hamiltonians By Adding Two Heisenberg Hamentioning
confidence: 99%
“…Examples of periodic and non-periodic orbits for this pasted potential are given in figure 2. For 'global' superintegrable systems all the bounded motions are periodic and the trajectories look like deformed Lissajous curves [10,11]. We should remark that such trajectories are smooth and they do not present 'angles' when crossing the boundary of a domain.…”
Section: (A) Superintegrable Hamiltonians By Adding Two Heisenberg Hamentioning
confidence: 99%
“…In this section we review the Hamiltonian (1.1) from the classical factorization viewpoint introduced in [15][16][17][18]. Although the results here presented are quite elementary, they are useful in order to present the approach that we will follow in the curved case.…”
Section: The Classical Factorization Methodsmentioning
confidence: 99%
“…In order to get a unified approach to find the symmetries for both, the classical and quantum systems, we have applied a factorization approach [15,18,36,44]. This method turns out to be helpful in order to highlight the correspondence between the classical and quantum algebraic symmetries.…”
Section: Discussionmentioning
confidence: 99%
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“…Our aim is to find additional constants of motion by means of the factorization method in order to show the maximal superintegrability of the system. We recall that the application of the factorisation method to the classical realm was first proposed in [12] and then developed in [13], [14], [15], [16], [17], [18]. A first pair of constants X ± will be obtained from the effective Hamiltonians H ξ and H θ , and a second pair Y ± from the next two effective Hamiltonians, H θ and H ϕ .…”
Section: Constants Of Motionmentioning
confidence: 99%