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Program - Brookhaven National Laboratory

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Correlations Between Nuclear Charge Radii, E0 Transitions and Summed M1 Strengths<br />

P. Van Isacker<br />

GANIL, CEA/DSM-CNRS/IN2P3, BP 55027, F-14076 Caen Cedex 5, France<br />

A systematic study of energy spectra throughout the rare-earth region (even-even nuclei from 58Ce to 74W)<br />

is carried out in the framework of the interacting boson model (IBM), which gives a global description of the<br />

spherical-to-deformed shape transition in the different isotopic chains. The resulting IBM Hamiltonian is<br />

then used for the calculation of nuclear charge radii (including isotope and isomer shifts) and E0 transitions<br />

with consistent operators for the two observables [1,2]. Following ideas developed by Ginocchio [3], an<br />

additional correlation is pointed out between both of these properties (i.e., charge radii and E0 transitions)<br />

with the summed M1 strength from the ground state of even-even nuclei to the scissors mode. This leads to<br />

correlation plots between isotope shifts and summed M1 strength differences on the one hand, and between<br />

ρ 2 (E0) values and summed M1 strengths on the other hand. Examples of such correlation plots are shown<br />

for rare-earth nuclei.<br />

[1] S. Zerguine, P. Van Isacker, A. Bouldjedri, and S. Heinze, Phys. Rev. Lett. 101, 022502 (2008). [2] S.<br />

Zerguine, P. Van Isacker, and A. Bouldjedri, Phys. Rev. C 85, 034331 (2012). [3] J.N. Ginocchio, Phys.<br />

Lett. B 265, 6 (1991).<br />

DD 4 4:40 PM<br />

First Total Absorption Spectroscopy Measurement of the Beta Decay of 139 Xe<br />

A. Fijalkowska, M. Karny, K. Mienik, Faculty of Physics, University of Warsaw, Warsaw, PL 00-681,<br />

Poland. K.P. Rykaczewski, M. Wolinska-Cichocka, C.J. Gross, J. W. Johnson, C. Jost, D. Stracener,<br />

ORNL, Oak Ridge, TN 37830, USA,. R.K. Grzywacz, L. Cartegni, K.C. Goetz, M. Al-Shudifat,<br />

University of Tennessee, Knoxville, TN 37996, USA. R. Goans, M. Madurga, D. Miller, S.W. Padgett,<br />

S.V. Paulauskas, E. Spejewski, ORAU, Oak Ridge, TN 37830, USA. B.C. Rasco, E. Zganjar, Louisiana<br />

State University, Baton Rouge, LA 70803, USA. J.H. Hamilton, A.V. Ramayya, Dept. of Physics and<br />

Astronomy, Vanderbilt University, Nashville, TN 37235, USA.<br />

The Modular Total Absorption Spectrometer (MTAS) has been recently constructed and commissioned at<br />

the Holifield Radioactive Ion Beam Facility (HRIBF) at Oak Ridge <strong>National</strong> <strong>Laboratory</strong> [1]. The main<br />

scientific goal of MTAS is to determine the true beta-decay feeding and following gamma radiation pattern<br />

for the decays of fission products. This is important not only for understanding of the relevant nuclear<br />

structure and beta decay processes, but also for the determination of the decay heat release during a<br />

nuclear fuel cycle. Existing theoretical simulations of decay heat show, in fact, significant deviations from<br />

experimental data [2-4]. These discrepancies are believed to be partially due to the incorrect or incomplete<br />

beta decay schemes. In this contribution we would like to present the results of the measurement of 139 Xe<br />

beta decay, which was identified among ”most wanted” for the analysis of decay heat in nuclear reactors<br />

[2]. 139 Xe nuclei, among others [5], were produced at HRIBF in the proton-induced fission of 238 U, mass<br />

separated and implanted onto a moving tape, which periodically transported the activity to the centre of<br />

MTAS. The results and their impact on the decay heat calculations will be presented and discussed.<br />

[1] M.Wolinska-Cichocka et al., contribution to this conference [2] “Assessment of fission product decay<br />

data for decay heat calculations” OECD 2007, NEA No 6284, vol. 25, ISBN 978-92-64-99034-0 [3] A.<br />

Algora et al., Phys. Rev. Lett., 105, 202501, 2010. [4] K. P. Rykaczewski, Physics 3, 94, 2010. [5] M.<br />

Karny et al., contribution to this conference.<br />

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