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Interplay between shape-phase transitions and shape coexistence in the Zr isotopes
Nuclear Theory · Submitted 18 Sep 2019
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We demonstrate the role of two concurrent types of quantum phase transitions, sharing a common critical point.
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The abstract, sentence by sentence
We investigate the evolution of structure in the zirconium isotopes where one of the most complex situations encountered in nuclear physics occurs. We demonstrate the role of two concurrent types of quantum phase transitions, sharing a common critical point. The first type, involves an abrupt crossing of coexisting normal and intruder configurations. The second type, involves a gradual shape-phase transition within the intruder configuration, changing from weakly-deformed to prolate-deformed and finally to gamma-unstable. Evidence for this scenario is provided by a detailed comparison with experimental data, using a definite algebraic framework.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We investigate the evolution of structure in the zirconium isotopes where one of the most complex situations encountered in nuclear physics occurs. | background 0.60 | 0.54 | 0.04 | asserted 0.92 |
| s1 | We demonstrate the role of two concurrent types of quantum phase transitions, sharing a common critical point. | result 0.68 | 0.91 | 0.63 | asserted 1.00 |
| s2 | The first type, involves an abrupt crossing of coexisting normal and intruder configurations. | result 0.83 | 0.56 | 0.16 | asserted 0.98 |
| s3 | The second type, involves a gradual shape-phase transition within the intruder configuration, changing from weakly-deformed to prolate-deformed and finally to gamma-unstable. | result 0.90 | 0.73 | 0.20 | asserted 1.00 |
| s4 | Evidence for this scenario is provided by a detailed comparison with experimental data, using a definite algebraic framework. | method 0.78 | 0.87 | 0.09 | asserted 0.97 |
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The paper
Original abstract
We investigate the evolution of structure in the zirconium isotopes where one of the most complex situations encountered in nuclear physics occurs. We demonstrate the role of two concurrent types of quantum phase transitions, sharing a common critical point. The first type, involves an abrupt crossing of coexisting normal and intruder configurations. The second type, involves a gradual shape-phase transition within the intruder configuration, changing from weakly-deformed to prolate-deformed and finally to gamma-unstable. Evidence for this scenario is provided by a detailed comparison with experimental data, using a definite algebraic framework.
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States the same result 5 papers
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We demonstrate the relevance of IQPTs to the Zr isotopes, with such coexisting Type I and Type II QPTs, and ground state shapes changing from spherical to prolate axially deformed and finally to gamma-unstable.
Intertwined Quantum Phase Transitions in the Zr Isotopes · 0.99
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The good agreement of our calculation with the vast empirical data along the chain of isotopes demonstrates the relevance of IQPTs to the zirconium isotopes, and can serve as a case study to set path for new investigations of IQPTs in other nuclei and other physical systems.
Zr Isotopes as a region of intertwined quantum phase transitions · 0.97
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The results suggest a remarkable interplay of multiple quantum phase transitions (QPTs).
Multiple quantum phase transitions in the Zr isotopes · 0.95
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A detailed analysis in the framework of the interacting boson model with configuration mixing, provides evidence for this scenario in the Zr isotopes.
Intertwined quantum phase transitions in the Zr chain · 0.90
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The algebraic framework of the interacting boson model with configuration mixing is employed to demonstrate the occurrence of intertwined quantum phase transitions (IQPTs) in the $_{40}$Zr isotopes with neutron number 52-70.
An algebraic approach to intertwined quantum phase transitions in the Zr isotopes · 0.88
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