2017
DOI: 10.1063/1.4972356
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Shape phase transition in γ-rigid prolate nuclei

Abstract: Abstract. A γ-rigid prolate version of the Bohr-Hamiltonian is quasi-exactly solved for a sextic oscillator potential. Both energies and wave functions are obtained in analytical form depending, up to a scale factor, on a single free parameter. Moreover, due to the special properties of the sextic potential, a shape evolution can be covered from a γ-rigid prolate harmonic vibrator to an anharmonic one crossing a critical region where the potential is flat.

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(1 citation statement)
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“…Since its inception in 1980 [4,5], the QES models have received great attention in the field of quantum mechanics due to its wide use in modeling many physical phenomena ( [2] and references therein). Increasing interest has been noticed for getting analytical solutions [6][7][8][9][10] as well as highly accurate approximations [11][12][13][14][15][16] of various models involving QES potentials. While several existing methods provide excellent results for specific cases, an efficient scheme for obtaining energy eigenvalues and eigenfunctions simultaneously for any QES model is of great demand.…”
Section: Introductionmentioning
confidence: 99%
“…Since its inception in 1980 [4,5], the QES models have received great attention in the field of quantum mechanics due to its wide use in modeling many physical phenomena ( [2] and references therein). Increasing interest has been noticed for getting analytical solutions [6][7][8][9][10] as well as highly accurate approximations [11][12][13][14][15][16] of various models involving QES potentials. While several existing methods provide excellent results for specific cases, an efficient scheme for obtaining energy eigenvalues and eigenfunctions simultaneously for any QES model is of great demand.…”
Section: Introductionmentioning
confidence: 99%