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Shape coexistence revealed in the N=Z isotope 72Kr through inelastic scattering
The N = Z = 36 nucleus 72 Kr has been studied by inelastic scattering at intermediate energies. Two targets, 9 Be and 197 Au, were used to extract the nuclear deformation length, δ N , and the reduced E 2 transition probability, B ( E 2). The previously unknown non-yrast 2 + and 4 + states as well a...
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Published in: | The European physical journal. A, Hadrons and nuclei Hadrons and nuclei, 2020, Vol.56 (6) |
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creator | Wimmer, K. Arici, T. Korten, W. Doornenbal, P. Delaroche, J.-P. Girod, M. Libert, J. Rodríguez, T. R. Aguilera, P. Algora, A. Ando, T. Baba, H. Blank, B. Boso, A. Chen, S. Corsi, A. Davies, P. de Angelis, G. de France, G. Doherty, D. T. Gerl, J. Gernhäuser, R. Goigoux, T. Jenkins, D. Kiss, G. Koyama, S. Motobayashi, T. Nagamine, S. Niikura, M. Nishimura, S. Obertelli, A. Lubos, D. Phong, V. H. Rubio, B. Sahin, E. Saito, T. Y. Sakurai, H. Sinclair, L. Steppenbeck, D. Taniuchi, R. Vaquero, V. Wadsworth, R. Wu, J. Zielinska, M. |
description | The
N
=
Z
=
36
nucleus
72
Kr has been studied by inelastic scattering at intermediate energies. Two targets,
9
Be and
197
Au, were used to extract the nuclear deformation length,
δ
N
, and the reduced
E
2 transition probability,
B
(
E
2). The previously unknown non-yrast
2
+
and
4
+
states as well as a new candidate for the octupole
3
-
state have been observed in the scattering on the Be target and placed in the level scheme based on
γ
-
γ
coincidences. The second
2
+
state was also observed in the scattering on the Au target and the
B
(
E
2
;
2
2
+
→
0
1
+
)
value could be determined for the first time. Analyzing the results in terms of a two-band mixing model shows clear evidence for a oblate-prolate shape coexistence and can be explained by a shape change from an oblate ground state to prolate deformed yrast band from the first
2
+
state. This interpretation is corroborated by beyond mean field calculations using the Gogny D1S interaction. |
doi_str_mv | 10.1140/epja/s10050-020-00171-3 |
format | article |
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N
=
Z
=
36
nucleus
72
Kr has been studied by inelastic scattering at intermediate energies. Two targets,
9
Be and
197
Au, were used to extract the nuclear deformation length,
δ
N
, and the reduced
E
2 transition probability,
B
(
E
2). The previously unknown non-yrast
2
+
and
4
+
states as well as a new candidate for the octupole
3
-
state have been observed in the scattering on the Be target and placed in the level scheme based on
γ
-
γ
coincidences. The second
2
+
state was also observed in the scattering on the Au target and the
B
(
E
2
;
2
2
+
→
0
1
+
)
value could be determined for the first time. Analyzing the results in terms of a two-band mixing model shows clear evidence for a oblate-prolate shape coexistence and can be explained by a shape change from an oblate ground state to prolate deformed yrast band from the first
2
+
state. This interpretation is corroborated by beyond mean field calculations using the Gogny D1S interaction.</description><identifier>ISSN: 1434-6001</identifier><identifier>EISSN: 1434-601X</identifier><identifier>DOI: 10.1140/epja/s10050-020-00171-3</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Hadrons ; Heavy Ions ; Inelastic scattering ; Nuclear deformation ; Nuclear Fusion ; Nuclear Physics ; Particle and Nuclear Physics ; Physics ; Physics and Astronomy ; Regular Article - Experimental Physics ; Transition probabilities</subject><ispartof>The European physical journal. A, Hadrons and nuclei, 2020, Vol.56 (6)</ispartof><rights>Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2020</rights><rights>Società Italiana di Fisica and Springer-Verlag GmbH Germany, part of Springer Nature 2020.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0001-8178-0405</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>315,786,790,27957,27958</link.rule.ids></links><search><creatorcontrib>Wimmer, K.</creatorcontrib><creatorcontrib>Arici, T.</creatorcontrib><creatorcontrib>Korten, W.</creatorcontrib><creatorcontrib>Doornenbal, P.</creatorcontrib><creatorcontrib>Delaroche, J.-P.</creatorcontrib><creatorcontrib>Girod, M.</creatorcontrib><creatorcontrib>Libert, J.</creatorcontrib><creatorcontrib>Rodríguez, T. R.</creatorcontrib><creatorcontrib>Aguilera, P.</creatorcontrib><creatorcontrib>Algora, A.</creatorcontrib><creatorcontrib>Ando, T.</creatorcontrib><creatorcontrib>Baba, H.</creatorcontrib><creatorcontrib>Blank, B.</creatorcontrib><creatorcontrib>Boso, A.</creatorcontrib><creatorcontrib>Chen, S.</creatorcontrib><creatorcontrib>Corsi, A.</creatorcontrib><creatorcontrib>Davies, P.</creatorcontrib><creatorcontrib>de Angelis, G.</creatorcontrib><creatorcontrib>de France, G.</creatorcontrib><creatorcontrib>Doherty, D. T.</creatorcontrib><creatorcontrib>Gerl, J.</creatorcontrib><creatorcontrib>Gernhäuser, R.</creatorcontrib><creatorcontrib>Goigoux, T.</creatorcontrib><creatorcontrib>Jenkins, D.</creatorcontrib><creatorcontrib>Kiss, G.</creatorcontrib><creatorcontrib>Koyama, S.</creatorcontrib><creatorcontrib>Motobayashi, T.</creatorcontrib><creatorcontrib>Nagamine, S.</creatorcontrib><creatorcontrib>Niikura, M.</creatorcontrib><creatorcontrib>Nishimura, S.</creatorcontrib><creatorcontrib>Obertelli, A.</creatorcontrib><creatorcontrib>Lubos, D.</creatorcontrib><creatorcontrib>Phong, V. H.</creatorcontrib><creatorcontrib>Rubio, B.</creatorcontrib><creatorcontrib>Sahin, E.</creatorcontrib><creatorcontrib>Saito, T. Y.</creatorcontrib><creatorcontrib>Sakurai, H.</creatorcontrib><creatorcontrib>Sinclair, L.</creatorcontrib><creatorcontrib>Steppenbeck, D.</creatorcontrib><creatorcontrib>Taniuchi, R.</creatorcontrib><creatorcontrib>Vaquero, V.</creatorcontrib><creatorcontrib>Wadsworth, R.</creatorcontrib><creatorcontrib>Wu, J.</creatorcontrib><creatorcontrib>Zielinska, M.</creatorcontrib><title>Shape coexistence revealed in the N=Z isotope 72Kr through inelastic scattering</title><title>The European physical journal. A, Hadrons and nuclei</title><addtitle>Eur. Phys. J. A</addtitle><description>The
N
=
Z
=
36
nucleus
72
Kr has been studied by inelastic scattering at intermediate energies. Two targets,
9
Be and
197
Au, were used to extract the nuclear deformation length,
δ
N
, and the reduced
E
2 transition probability,
B
(
E
2). The previously unknown non-yrast
2
+
and
4
+
states as well as a new candidate for the octupole
3
-
state have been observed in the scattering on the Be target and placed in the level scheme based on
γ
-
γ
coincidences. The second
2
+
state was also observed in the scattering on the Au target and the
B
(
E
2
;
2
2
+
→
0
1
+
)
value could be determined for the first time. Analyzing the results in terms of a two-band mixing model shows clear evidence for a oblate-prolate shape coexistence and can be explained by a shape change from an oblate ground state to prolate deformed yrast band from the first
2
+
state. This interpretation is corroborated by beyond mean field calculations using the Gogny D1S interaction.</description><subject>Hadrons</subject><subject>Heavy Ions</subject><subject>Inelastic scattering</subject><subject>Nuclear deformation</subject><subject>Nuclear Fusion</subject><subject>Nuclear Physics</subject><subject>Particle and Nuclear Physics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Regular Article - Experimental Physics</subject><subject>Transition probabilities</subject><issn>1434-6001</issn><issn>1434-601X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNpFkEtLw0AQgBdRsFZ_gwHPsTP7bA4epPjCYg_2IF6WTTJtU0oSd7fiz3djRQ_DDDMfM8PH2CXCNaKECfVbNwkIoCAHngLQYC6O2AilkLkGfDv-qwFP2VkIWwCQvNAjtnjduJ6yqqOvJkRqK8o8fZLbUZ01bRY3lL3cvGdN6GKXOMOffWr6br_epDntXIhNlYXKxUi-adfn7GTldoEufvOYLe_vlrPHfL54eJrdzvPeGJGrKRJoKI2SpZDARQWcl9wUK1nAtAStnHNAAg1Uiora1bUrSoXGOA0GUIzZ1WFt77uPPYVot93et-mi5RIKjkprnajpgQr98Bv5fwrBDvbsYM8e7Nlkz_7Ys0J8A7bPYw4</recordid><startdate>2020</startdate><enddate>2020</enddate><creator>Wimmer, K.</creator><creator>Arici, T.</creator><creator>Korten, W.</creator><creator>Doornenbal, P.</creator><creator>Delaroche, J.-P.</creator><creator>Girod, M.</creator><creator>Libert, J.</creator><creator>Rodríguez, T. R.</creator><creator>Aguilera, P.</creator><creator>Algora, A.</creator><creator>Ando, T.</creator><creator>Baba, H.</creator><creator>Blank, B.</creator><creator>Boso, A.</creator><creator>Chen, S.</creator><creator>Corsi, A.</creator><creator>Davies, P.</creator><creator>de Angelis, G.</creator><creator>de France, G.</creator><creator>Doherty, D. T.</creator><creator>Gerl, J.</creator><creator>Gernhäuser, R.</creator><creator>Goigoux, T.</creator><creator>Jenkins, D.</creator><creator>Kiss, G.</creator><creator>Koyama, S.</creator><creator>Motobayashi, T.</creator><creator>Nagamine, S.</creator><creator>Niikura, M.</creator><creator>Nishimura, S.</creator><creator>Obertelli, A.</creator><creator>Lubos, D.</creator><creator>Phong, V. H.</creator><creator>Rubio, B.</creator><creator>Sahin, E.</creator><creator>Saito, T. Y.</creator><creator>Sakurai, H.</creator><creator>Sinclair, L.</creator><creator>Steppenbeck, D.</creator><creator>Taniuchi, R.</creator><creator>Vaquero, V.</creator><creator>Wadsworth, R.</creator><creator>Wu, J.</creator><creator>Zielinska, M.</creator><general>Springer Berlin Heidelberg</general><general>Springer Nature B.V</general><scope/><orcidid>https://orcid.org/0000-0001-8178-0405</orcidid></search><sort><creationdate>2020</creationdate><title>Shape coexistence revealed in the N=Z isotope 72Kr through inelastic scattering</title><author>Wimmer, K. ; Arici, T. ; Korten, W. ; Doornenbal, P. ; Delaroche, J.-P. ; Girod, M. ; Libert, J. ; Rodríguez, T. R. ; Aguilera, P. ; Algora, A. ; Ando, T. ; Baba, H. ; Blank, B. ; Boso, A. ; Chen, S. ; Corsi, A. ; Davies, P. ; de Angelis, G. ; de France, G. ; Doherty, D. T. ; Gerl, J. ; Gernhäuser, R. ; Goigoux, T. ; Jenkins, D. ; Kiss, G. ; Koyama, S. ; Motobayashi, T. ; Nagamine, S. ; Niikura, M. ; Nishimura, S. ; Obertelli, A. ; Lubos, D. ; Phong, V. H. ; Rubio, B. ; Sahin, E. ; Saito, T. Y. ; Sakurai, H. ; Sinclair, L. ; Steppenbeck, D. ; Taniuchi, R. ; Vaquero, V. ; Wadsworth, R. ; Wu, J. ; Zielinska, M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p773-581e060b754b34023c022b279f4908b065aaa0e3170c5e9dadda9b5177a607013</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Hadrons</topic><topic>Heavy Ions</topic><topic>Inelastic scattering</topic><topic>Nuclear deformation</topic><topic>Nuclear Fusion</topic><topic>Nuclear Physics</topic><topic>Particle and Nuclear Physics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Regular Article - Experimental Physics</topic><topic>Transition probabilities</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wimmer, K.</creatorcontrib><creatorcontrib>Arici, T.</creatorcontrib><creatorcontrib>Korten, W.</creatorcontrib><creatorcontrib>Doornenbal, P.</creatorcontrib><creatorcontrib>Delaroche, J.-P.</creatorcontrib><creatorcontrib>Girod, M.</creatorcontrib><creatorcontrib>Libert, J.</creatorcontrib><creatorcontrib>Rodríguez, T. R.</creatorcontrib><creatorcontrib>Aguilera, P.</creatorcontrib><creatorcontrib>Algora, A.</creatorcontrib><creatorcontrib>Ando, T.</creatorcontrib><creatorcontrib>Baba, H.</creatorcontrib><creatorcontrib>Blank, B.</creatorcontrib><creatorcontrib>Boso, A.</creatorcontrib><creatorcontrib>Chen, S.</creatorcontrib><creatorcontrib>Corsi, A.</creatorcontrib><creatorcontrib>Davies, P.</creatorcontrib><creatorcontrib>de Angelis, G.</creatorcontrib><creatorcontrib>de France, G.</creatorcontrib><creatorcontrib>Doherty, D. T.</creatorcontrib><creatorcontrib>Gerl, J.</creatorcontrib><creatorcontrib>Gernhäuser, R.</creatorcontrib><creatorcontrib>Goigoux, T.</creatorcontrib><creatorcontrib>Jenkins, D.</creatorcontrib><creatorcontrib>Kiss, G.</creatorcontrib><creatorcontrib>Koyama, S.</creatorcontrib><creatorcontrib>Motobayashi, T.</creatorcontrib><creatorcontrib>Nagamine, S.</creatorcontrib><creatorcontrib>Niikura, M.</creatorcontrib><creatorcontrib>Nishimura, S.</creatorcontrib><creatorcontrib>Obertelli, A.</creatorcontrib><creatorcontrib>Lubos, D.</creatorcontrib><creatorcontrib>Phong, V. H.</creatorcontrib><creatorcontrib>Rubio, B.</creatorcontrib><creatorcontrib>Sahin, E.</creatorcontrib><creatorcontrib>Saito, T. Y.</creatorcontrib><creatorcontrib>Sakurai, H.</creatorcontrib><creatorcontrib>Sinclair, L.</creatorcontrib><creatorcontrib>Steppenbeck, D.</creatorcontrib><creatorcontrib>Taniuchi, R.</creatorcontrib><creatorcontrib>Vaquero, V.</creatorcontrib><creatorcontrib>Wadsworth, R.</creatorcontrib><creatorcontrib>Wu, J.</creatorcontrib><creatorcontrib>Zielinska, M.</creatorcontrib><jtitle>The European physical journal. A, Hadrons and nuclei</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Wimmer, K.</au><au>Arici, T.</au><au>Korten, W.</au><au>Doornenbal, P.</au><au>Delaroche, J.-P.</au><au>Girod, M.</au><au>Libert, J.</au><au>Rodríguez, T. R.</au><au>Aguilera, P.</au><au>Algora, A.</au><au>Ando, T.</au><au>Baba, H.</au><au>Blank, B.</au><au>Boso, A.</au><au>Chen, S.</au><au>Corsi, A.</au><au>Davies, P.</au><au>de Angelis, G.</au><au>de France, G.</au><au>Doherty, D. T.</au><au>Gerl, J.</au><au>Gernhäuser, R.</au><au>Goigoux, T.</au><au>Jenkins, D.</au><au>Kiss, G.</au><au>Koyama, S.</au><au>Motobayashi, T.</au><au>Nagamine, S.</au><au>Niikura, M.</au><au>Nishimura, S.</au><au>Obertelli, A.</au><au>Lubos, D.</au><au>Phong, V. H.</au><au>Rubio, B.</au><au>Sahin, E.</au><au>Saito, T. Y.</au><au>Sakurai, H.</au><au>Sinclair, L.</au><au>Steppenbeck, D.</au><au>Taniuchi, R.</au><au>Vaquero, V.</au><au>Wadsworth, R.</au><au>Wu, J.</au><au>Zielinska, M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Shape coexistence revealed in the N=Z isotope 72Kr through inelastic scattering</atitle><jtitle>The European physical journal. A, Hadrons and nuclei</jtitle><stitle>Eur. Phys. J. A</stitle><date>2020</date><risdate>2020</risdate><volume>56</volume><issue>6</issue><issn>1434-6001</issn><eissn>1434-601X</eissn><abstract>The
N
=
Z
=
36
nucleus
72
Kr has been studied by inelastic scattering at intermediate energies. Two targets,
9
Be and
197
Au, were used to extract the nuclear deformation length,
δ
N
, and the reduced
E
2 transition probability,
B
(
E
2). The previously unknown non-yrast
2
+
and
4
+
states as well as a new candidate for the octupole
3
-
state have been observed in the scattering on the Be target and placed in the level scheme based on
γ
-
γ
coincidences. The second
2
+
state was also observed in the scattering on the Au target and the
B
(
E
2
;
2
2
+
→
0
1
+
)
value could be determined for the first time. Analyzing the results in terms of a two-band mixing model shows clear evidence for a oblate-prolate shape coexistence and can be explained by a shape change from an oblate ground state to prolate deformed yrast band from the first
2
+
state. This interpretation is corroborated by beyond mean field calculations using the Gogny D1S interaction.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1140/epja/s10050-020-00171-3</doi><orcidid>https://orcid.org/0000-0001-8178-0405</orcidid></addata></record> |
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language | eng |
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source | Springer Link |
subjects | Hadrons Heavy Ions Inelastic scattering Nuclear deformation Nuclear Fusion Nuclear Physics Particle and Nuclear Physics Physics Physics and Astronomy Regular Article - Experimental Physics Transition probabilities |
title | Shape coexistence revealed in the N=Z isotope 72Kr through inelastic scattering |
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