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arXiv:1207.3496 · AIP conference proceedings

Regular and chaotic classical dynamics in the U(5)-SU(3) quantum phase transition of the IBM

Michal Macek, A. Leviatan

Published Jan 1, 2012• 0 citations
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Abstract

We study the classical dynamics in a generic first-order quantum phase transition between the U(5) and SU(3) limits of the interacting boson model. The dynamics is chaotic, of Hénon-Heiles type, in the spherical phase and is regular, yet sensitive to local degeneracies, in the deformed phase. Both types of dynamics persist in the coexistence region resulting in a divided phase space.

DOI
10.1063/1.4759429

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We study the classical dynamics in a generic first-order quantum phase transition between the U(5) and SU(3) limits of the interacting boson model. The dynamics is chaotic, of Hénon-Heiles type, in the spherical phase and is regular, yet sensitive to local degeneracies, in the deformed phase. Both types of dynamics persist in the coexistence region resulting in a divided phase space.
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First order quantum phase transition (QPT) between spherical and axially deformed nuclei shows coexisting, but well-separated regions of regular and chaotic dynamics. We employ a Hamiltonian of the Arima-Iachello Interacting Boson Model (IBM) with an arbitrarily high potential barrier separating the phases. Classical and quantum analyses reveal markedly distinct behavior of the two phases: Deformed phase is completely regular, while the spherical phase shows highly chaotic dynamics, similar to the Hénon-Heiles system. Rotational bands with quasi-SU(3) characteristics built upon the regular vibrational spectrum of beta- and gamma-vibrations are observed in the deformed phase up to very high excitation energies.
We study the interplay between regular and chaotic dynamics at the critical point of a generic first-order quantum phase transition in an interacting boson model of nuclei. A classical analysis reveals a distinct behavior of the coexisting phases in a broad energy range. The dynamics is completely regular in the deformed phase and, simultaneously, strongly chaotic in the spherical phase. A quantum analysis of the spectra separates the regular states from the irregular ones, assigns them to particular phases, and discloses persisting regular rotational bands in the deformed region.
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Symmetry-Reduced Variational Quantum Simulation of the U(5)→SU(3)U(5)\rightarrow SU(3)U(5)→SU(3) Quantum Phase Transition in the Interacting Boson Model
The spherical-to-deformed quantum phase transition of the Interacting Boson Model (IBM) is investigated using the variational quantum eigensolver (VQE). The U(5)U(5)U(5)--SU(3)SU(3)SU(3) transitional Hamiltonian is studied with χ=−7/2χ=-\sqrt{7}/2χ=−7​/2. We develop a symmetry-preserving, minimum-qubit VQE framework for collective nuclear models, achieving a substantial reduction in qubit requirements without compromising the finite-size quantum-phase-transition physics. The transition is characterized through the normalized ddd-boson occupation and ground-state energy derivatives. Finite-size results are found to approach the analytic critical point ξc=8/17≃0.470588ξ_c=8/17\simeq0.470588ξc​=8/17≃0.470588, with an independent order-parameter extrapolation yielding ξ∞=0.46986(61)ξ_\infty=0.46986(61)ξ∞​=0.46986(61). The VQE reproduces ground-state energies and structural observables to numerical precision. These results demonstrate the potential of symmetry-reduced VQE for efficient quantum simulations of collective nuclear dynamics and quantum phase transitions.