Islands of Shape Coexistence: Theoretical Predictions and Experimental Evidence

Parameter-free theoretical predictions based on a dual shell mechanism within the proxy-SU(3) symmetry of atomic nuclei, as well as covariant density functional theory calculations using the DDME2 functional indicate that shape coexistence (SC) based on the particle-hole excitation mechanism cannot...

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Main Authors: Andriana Martinou, Dennis Bonatsos, Spyridon Kosmas Peroulis, Konstantinos Eleftherios Karakatsanis, Theodoros John Mertzimekis, Nikolay Minkov
Format: Article
Language:English
Published: MDPI AG 2022-12-01
Series:Symmetry
Subjects:
Online Access:https://www.mdpi.com/2073-8994/15/1/29
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author Andriana Martinou
Dennis Bonatsos
Spyridon Kosmas Peroulis
Konstantinos Eleftherios Karakatsanis
Theodoros John Mertzimekis
Nikolay Minkov
author_facet Andriana Martinou
Dennis Bonatsos
Spyridon Kosmas Peroulis
Konstantinos Eleftherios Karakatsanis
Theodoros John Mertzimekis
Nikolay Minkov
author_sort Andriana Martinou
collection DOAJ
description Parameter-free theoretical predictions based on a dual shell mechanism within the proxy-SU(3) symmetry of atomic nuclei, as well as covariant density functional theory calculations using the DDME2 functional indicate that shape coexistence (SC) based on the particle-hole excitation mechanism cannot occur everywhere on the nuclear chart but is restricted on islands lying within regions of 7–8, 17–20, 34–40, 59–70, 96–112, 146–168 protons or neutrons. Systematics of data for even-even nuclei possessing <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>K</mi><mo>=</mo><mn>0</mn></mrow></semantics></math></inline-formula> (beta) and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>K</mi><mo>=</mo><mn>2</mn></mrow></semantics></math></inline-formula> (gamma) bands support the existence of these islands, on which shape coexistence appears whenever the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>K</mi><mo>=</mo><mn>0</mn></mrow></semantics></math></inline-formula> bandhead <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msubsup><mn>0</mn><mn>2</mn><mo>+</mo></msubsup></semantics></math></inline-formula> and the first excited state of the ground state band <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msubsup><mn>2</mn><mn>1</mn><mo>+</mo></msubsup></semantics></math></inline-formula> lie close in energy, with nuclei characterized by <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msubsup><mn>0</mn><mn>2</mn><mo>+</mo></msubsup></semantics></math></inline-formula> lying below the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msubsup><mn>2</mn><mn>1</mn><mo>+</mo></msubsup></semantics></math></inline-formula> found in the center of these islands. In addition, a simple theoretical mechanism leading to multiple-shape coexistence is briefly discussed.
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spelling doaj.art-b30a8a8fec8a4b9cb08086e2e4dfa1b32023-12-01T00:50:41ZengMDPI AGSymmetry2073-89942022-12-011512910.3390/sym15010029Islands of Shape Coexistence: Theoretical Predictions and Experimental EvidenceAndriana Martinou0Dennis Bonatsos1Spyridon Kosmas Peroulis2Konstantinos Eleftherios Karakatsanis3Theodoros John Mertzimekis4Nikolay Minkov5Institute of Nuclear and Particle Physics, National Centre for Scientific Research “Demokritos”, GR-15310 Aghia Paraskevi, Attiki, GreeceInstitute of Nuclear and Particle Physics, National Centre for Scientific Research “Demokritos”, GR-15310 Aghia Paraskevi, Attiki, GreeceInstitute of Nuclear and Particle Physics, National Centre for Scientific Research “Demokritos”, GR-15310 Aghia Paraskevi, Attiki, GreeceDepartment of Physics, Faculty of Science, University of Zagreb, HR-10000 Zagreb, CroatiaDepartment of Physics, National and Kapodistrian University of Athens, Zografou Campus, GR-15784 Athens, GreeceInstitute of Nuclear Research and Nuclear Energy, Bulgarian Academy of Sciences, 72 Tzarigrad Road, 1784 Sofia, BulgariaParameter-free theoretical predictions based on a dual shell mechanism within the proxy-SU(3) symmetry of atomic nuclei, as well as covariant density functional theory calculations using the DDME2 functional indicate that shape coexistence (SC) based on the particle-hole excitation mechanism cannot occur everywhere on the nuclear chart but is restricted on islands lying within regions of 7–8, 17–20, 34–40, 59–70, 96–112, 146–168 protons or neutrons. Systematics of data for even-even nuclei possessing <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>K</mi><mo>=</mo><mn>0</mn></mrow></semantics></math></inline-formula> (beta) and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>K</mi><mo>=</mo><mn>2</mn></mrow></semantics></math></inline-formula> (gamma) bands support the existence of these islands, on which shape coexistence appears whenever the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>K</mi><mo>=</mo><mn>0</mn></mrow></semantics></math></inline-formula> bandhead <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msubsup><mn>0</mn><mn>2</mn><mo>+</mo></msubsup></semantics></math></inline-formula> and the first excited state of the ground state band <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msubsup><mn>2</mn><mn>1</mn><mo>+</mo></msubsup></semantics></math></inline-formula> lie close in energy, with nuclei characterized by <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msubsup><mn>0</mn><mn>2</mn><mo>+</mo></msubsup></semantics></math></inline-formula> lying below the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msubsup><mn>2</mn><mn>1</mn><mo>+</mo></msubsup></semantics></math></inline-formula> found in the center of these islands. In addition, a simple theoretical mechanism leading to multiple-shape coexistence is briefly discussed.https://www.mdpi.com/2073-8994/15/1/29shape coexistenceproxy-SU(3) symmetrycovariant density functional theory
spellingShingle Andriana Martinou
Dennis Bonatsos
Spyridon Kosmas Peroulis
Konstantinos Eleftherios Karakatsanis
Theodoros John Mertzimekis
Nikolay Minkov
Islands of Shape Coexistence: Theoretical Predictions and Experimental Evidence
Symmetry
shape coexistence
proxy-SU(3) symmetry
covariant density functional theory
title Islands of Shape Coexistence: Theoretical Predictions and Experimental Evidence
title_full Islands of Shape Coexistence: Theoretical Predictions and Experimental Evidence
title_fullStr Islands of Shape Coexistence: Theoretical Predictions and Experimental Evidence
title_full_unstemmed Islands of Shape Coexistence: Theoretical Predictions and Experimental Evidence
title_short Islands of Shape Coexistence: Theoretical Predictions and Experimental Evidence
title_sort islands of shape coexistence theoretical predictions and experimental evidence
topic shape coexistence
proxy-SU(3) symmetry
covariant density functional theory
url https://www.mdpi.com/2073-8994/15/1/29
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