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WORLD SCIENTIFIC eBooks

Effective Hamiltonian in Algebraic Approach

Published Nov 1, 2000• 0 citations
Publisher
DOI
10.1142/9789812386328_0027

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Non-standard quantum algebras and finite dimensional $\mathcal{PT}$-symmetric systems

Ángel Ballesteros, Romina Ramírez, M. Reboiro

In this work, $\mathcal{PT}$-symmetric Hamiltonians defined on quantum $sl(2, \mathbb R)$ algebras are presented. We study the spectrum of a family of non-Hermitian Hamiltonians written in terms of the generators of the non-standard $U_{z}(sl(2, \mathbb R))$ Hopf algebra deformation of $sl(2, \mathbb R)$. By making use of a particular boson representation of the generators of $U_{z}(sl(2, \mathbb R))$, both the co-product and the commutation relations of the quantum algebra are shown to be invariant under the $\mathcal{PT}$-transformation. In terms of these operators, we construct several finite dimensional $\mathcal{PT}$-symmetry Hamiltonians, whose spectrum is analytically obtained for any arbitrary dimension. In particular, we show the appearance of Exceptional Points in the space of model parameters and we discuss the behaviour of the spectrum both in the exact $\mathcal{PT}$-symmetry and the broken $\mathcal{PT}$-symmetry dynamical phases. As an application, we show that this non-standard quantum algebra can be used to define an effective model Hamiltonian describing accurately the experimental spectra of three-electron hybrid qubits based on asymmetric double quantum dots. Remarkably enough, in this effective model, the deformation parameter $z$ has to be identified with the detuning parameter of the system.

arXiv:2309.15305•Sep 26, 2023•0 citations
We show that the Stark and Kerr Hamiltonians are deeply connected in the framework of dynamical algebras. We found that the algebras for both Hamiltonians are the same when physically relevant magnitudes, such as the population inversion and the nnnth order coherence function are considered as elements of a Lie algebra under commutation with the Hamiltonians. By analyzing the equations of motion we were able to find a set of conditions for the characteristic magnitudes of both Hamiltonians that leads to the same dynamical behavior for all the elements of the group. Finally, we conclude that the results of this paper can be generalized to any extension of the Jaynes-Cummings model, where any of the different elements of the group are present.
Non-standard quantum algebras and finite dimensional PT\mathcal{PT}PT-symmetric systems
In this work, PT\mathcal{PT}PT-symmetric Hamiltonians defined on quantum sl(2,R)sl(2, \mathbb R)sl(2,R) algebras are presented. We study the spectrum of a family of non-Hermitian Hamiltonians written in terms of the generators of the non-standard Uz(sl(2,R))U_{z}(sl(2, \mathbb R))Uz​(sl(2,R)) Hopf algebra deformation of sl(2,R)sl(2, \mathbb R)sl(2,R). By making use of a particular boson representation of the generators of Uz(sl(2,R))U_{z}(sl(2, \mathbb R))Uz​(sl(2,R)), both the co-product and the commutation relations of the quantum algebra are shown to be invariant under the PT\mathcal{PT}PT-transformation. In terms of these operators, we construct several finite dimensional PT\mathcal{PT}PT-symmetry Hamiltonians, whose spectrum is analytically obtained for any arbitrary dimension. In particular, we show the appearance of Exceptional Points in the space of model parameters and we discuss the behaviour of the spectrum both in the exact PT\mathcal{PT}PT-symmetry and the broken PT\mathcal{PT}PT-symmetry dynamical phases. As an application, we show that this non-standard quantum algebra can be used to define an effective model Hamiltonian describing accurately the experimental spectra of three-electron hybrid qubits based on asymmetric double quantum dots. Remarkably enough, in this effective model, the deformation parameter zzz has to be identified with the detuning parameter of the system.