Abstract:We have constructed a Heisenberg-type algebra generated by the Hamiltonian, the step operators and an auxiliar operator. This algebra describes quantum systems having eigenvalues of the Hamiltonian depending on the eigenvalues of the two previous levels. This happens, for example, for systems having the energy spectrum given by Fibonacci sequence. Moreover, the algebraic structure depends on two functions f (x) and g(x). When these two functions are linear we classify, analysing the stability of the fixed poin… Show more
“…5, the thermo-statistical results for GL p,q (2)-and SU q 1 /q 2 (2)-invariant boson models having the model Hamiltonians in (17) and (23) are obviously different, since the nature of the two-parameter deformations of the quantum group invariant bosonic oscillator algebras for these models is quite different on the algebraic basis. The differences between these two-parameter realizations result not only from the defining commutation relations of both of the bosonic oscillator algebras in (1) and (2), but also from the Fock space representation properties of the two algebras.…”
Section: Discussionmentioning
confidence: 99%
“…Using the GL p,q (2)-invariant Hamiltonian in (17), the grand partition function in the high-temperature limit is…”
Section: High-temperature Thermodynamical Behaviours Of the Su Q 1 /Qmentioning
confidence: 99%
“…They have found many applications in a wide spectrum of research in physics. For instance, there are some possible connections between one-parameter deformed quantum groups and generalized statistical mechanics [7][8][9][10][11][12][13][14][15][16][17]. However, in the last few years, a considerable effort has been spent to studies on thermo-statistical properties of two-parameter generalized bosonic and fermionic oscillator gas models which are invariant under the actions of some specific quantum groups.…”
We discuss the algebras, representations, and thermodynamics of quantum group bosonic gas models with two different symmetries: GL p,q (2) and SU q 1 /q 2 (2). We establish the nature of the basic numbers which follow from these GL p,q (2)-and SU q 1 /q 2 (2)-invariant bosonic algebras. The Fock space representations of both of these quantum group invariant bosonic oscillator algebras are analyzed. It is concisely shown that these two quantum group invariant bosonic particle gases have different algebraic and high-temperature thermostatistical properties.
“…5, the thermo-statistical results for GL p,q (2)-and SU q 1 /q 2 (2)-invariant boson models having the model Hamiltonians in (17) and (23) are obviously different, since the nature of the two-parameter deformations of the quantum group invariant bosonic oscillator algebras for these models is quite different on the algebraic basis. The differences between these two-parameter realizations result not only from the defining commutation relations of both of the bosonic oscillator algebras in (1) and (2), but also from the Fock space representation properties of the two algebras.…”
Section: Discussionmentioning
confidence: 99%
“…Using the GL p,q (2)-invariant Hamiltonian in (17), the grand partition function in the high-temperature limit is…”
Section: High-temperature Thermodynamical Behaviours Of the Su Q 1 /Qmentioning
confidence: 99%
“…They have found many applications in a wide spectrum of research in physics. For instance, there are some possible connections between one-parameter deformed quantum groups and generalized statistical mechanics [7][8][9][10][11][12][13][14][15][16][17]. However, in the last few years, a considerable effort has been spent to studies on thermo-statistical properties of two-parameter generalized bosonic and fermionic oscillator gas models which are invariant under the actions of some specific quantum groups.…”
We discuss the algebras, representations, and thermodynamics of quantum group bosonic gas models with two different symmetries: GL p,q (2) and SU q 1 /q 2 (2). We establish the nature of the basic numbers which follow from these GL p,q (2)-and SU q 1 /q 2 (2)-invariant bosonic algebras. The Fock space representations of both of these quantum group invariant bosonic oscillator algebras are analyzed. It is concisely shown that these two quantum group invariant bosonic particle gases have different algebraic and high-temperature thermostatistical properties.
“…The first few terms of the Fibonacci sequence are: 0, 1, 1, 2, 3,5,8,13,21,34,55,89,144,233,377,610,987,1597,2584, . That is, F n D F n 1 C F n 2 for all n 2.…”
Consider the Fibonacci sequence ¹F n º 1 nD0 having initial conditions F 0 D 0, F 1 D 1 and recurrence relation F n D F n 1 CF n 2 .n 2/. The Fibonacci sequence has been generalized in many ways, some by preserving the initial conditions, and others by preserving the recurrence relation. In this article, we study a new generalization ¹q n º, with initial conditions q 0 D 0 and q 1 D 1 which is generated by the recurrence relation q n D aq n 1 C q n 2 (when n is even) or q n D bq n 1 C q n 2 (when n is odd), where a and b are nonzero real numbers. Some well-known sequences are special cases of this generalization. The Fibonacci sequence is a special case of ¹q n º with a D b D 1. Pell's sequence is ¹q n º with a D b D 2 and the k-Fibonacci sequence is ¹q n º with a D b D k. We produce an extended Binet's formula for the sequence ¹q n º and, thereby, identities such as Cassini's, Catalan's, d'Ocagne's, etc.
“…This algebra, called generalized Heisenberg algebra, depends on an analytical function f and the eigenvalues α n of the Hamiltonian are given by the one-step recurrence α n+1 = f (α n ). This structure has been used in different physical situations, see the references given in the recent paper [1]. In the same paper [1] de Souza et al introduced an extended two-step Heisenberg algebra having many interesting properties.…”
It is shown how some of the recent results of de Souza et al. [1] can be generalized to describe Hamiltonians whose eigenvalues are given as k-generalized Fibonacci numbers. Here k is an arbitrary integer and the cases considered by de Souza et al. corespond to k = 2.
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