Revised B(E3) transition rate and structure of the 3− level in 96Zr
The B(E3) transition strength from the 1897-keV, 3− level in 96Zr has been reevaluated from six high-statistics, independent data sets. The measured value of 42(3) W.u. is significantly lower than that adopted in recent compilations. It is, however, in line with the global systematics of collective...
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Elsevier
2019-01-01
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Series: | Physics Letters B |
Online Access: | http://www.sciencedirect.com/science/article/pii/S0370269318308943 |
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author | Ł.W. Iskra R. Broda R.V.F. Janssens M.P. Carpenter B. Fornal T. Lauritsen T. Otsuka T. Togashi Y. Tsunoda W.B. Walters S. Zhu |
author_facet | Ł.W. Iskra R. Broda R.V.F. Janssens M.P. Carpenter B. Fornal T. Lauritsen T. Otsuka T. Togashi Y. Tsunoda W.B. Walters S. Zhu |
author_sort | Ł.W. Iskra |
collection | DOAJ |
description | The B(E3) transition strength from the 1897-keV, 3− level in 96Zr has been reevaluated from six high-statistics, independent data sets. The measured value of 42(3) W.u. is significantly lower than that adopted in recent compilations. It is, however, in line with the global systematics of collective B(E3) rates found throughout the periodic table. Thus, the “exceptional” character of this transition, that challenged theory, no longer applies. Monte Carlo shell-model calculations indicate that the collectivity of the octupole vibration arises from both proton and neutron excitations involving a large number of orbitals. Keywords: 90≤A≤149, 3− level, Octupole excitation, Lifetimes and branching ratios, B(E3) strength, Monte Carlo shell model calculations |
first_indexed | 2024-12-12T18:16:55Z |
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id | doaj.art-18afb102db504b23b3a26344db9a34a3 |
institution | Directory Open Access Journal |
issn | 0370-2693 |
language | English |
last_indexed | 2024-12-12T18:16:55Z |
publishDate | 2019-01-01 |
publisher | Elsevier |
record_format | Article |
series | Physics Letters B |
spelling | doaj.art-18afb102db504b23b3a26344db9a34a32022-12-22T00:16:14ZengElsevierPhysics Letters B0370-26932019-01-01788396400Revised B(E3) transition rate and structure of the 3− level in 96ZrŁ.W. Iskra0R. Broda1R.V.F. Janssens2M.P. Carpenter3B. Fornal4T. Lauritsen5T. Otsuka6T. Togashi7Y. Tsunoda8W.B. Walters9S. Zhu10Institute of Nuclear Physics, PAN, 31-342 Kraków, Poland; Corresponding author at: Institute of Nuclear Physics, PAN, 31-342 Kraków, Poland.Institute of Nuclear Physics, PAN, 31-342 Kraków, PolandDepartment of Physics and Astronomy, University of North Carolina at Chapel Hill, Chapel Hill, NC 27599, USA; Triangle Universities Nuclear Laboratory, Duke University, Durham, NC 27708, USA; Corresponding author at: Department of Physics and Astronomy, University of North Carolina at Chapel Hill, Chapel Hill, NC 27599, USA.Physics Division, Argonne National Laboratory, Argonne, IL 60439, USAInstitute of Nuclear Physics, PAN, 31-342 Kraków, PolandPhysics Division, Argonne National Laboratory, Argonne, IL 60439, USACenter for Nuclear Study, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, JapanCenter for Nuclear Study, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, JapanCenter for Nuclear Study, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, JapanDepartment of Chemistry and Biochemistry, University of Maryland, College Park, MD 20742, USAPhysics Division, Argonne National Laboratory, Argonne, IL 60439, USAThe B(E3) transition strength from the 1897-keV, 3− level in 96Zr has been reevaluated from six high-statistics, independent data sets. The measured value of 42(3) W.u. is significantly lower than that adopted in recent compilations. It is, however, in line with the global systematics of collective B(E3) rates found throughout the periodic table. Thus, the “exceptional” character of this transition, that challenged theory, no longer applies. Monte Carlo shell-model calculations indicate that the collectivity of the octupole vibration arises from both proton and neutron excitations involving a large number of orbitals. Keywords: 90≤A≤149, 3− level, Octupole excitation, Lifetimes and branching ratios, B(E3) strength, Monte Carlo shell model calculationshttp://www.sciencedirect.com/science/article/pii/S0370269318308943 |
spellingShingle | Ł.W. Iskra R. Broda R.V.F. Janssens M.P. Carpenter B. Fornal T. Lauritsen T. Otsuka T. Togashi Y. Tsunoda W.B. Walters S. Zhu Revised B(E3) transition rate and structure of the 3− level in 96Zr Physics Letters B |
title | Revised B(E3) transition rate and structure of the 3− level in 96Zr |
title_full | Revised B(E3) transition rate and structure of the 3− level in 96Zr |
title_fullStr | Revised B(E3) transition rate and structure of the 3− level in 96Zr |
title_full_unstemmed | Revised B(E3) transition rate and structure of the 3− level in 96Zr |
title_short | Revised B(E3) transition rate and structure of the 3− level in 96Zr |
title_sort | revised b e3 transition rate and structure of the 3 level in 96zr |
url | http://www.sciencedirect.com/science/article/pii/S0370269318308943 |
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