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Z = 8 to Z = 98 nuclei and are compared to theory. A systematic difference of ∼ 5.5% has been identified,<br />

namely theory overestimates experiment. For routine use of the new table with BrIcc [2], we propose to<br />

assign a general uncertainty of 5.5% to the Ω(E) values.<br />

[1] I.M. Band, M.B. Trzhaskovskaya, C.W. Nestor, Jr., P.O. Tikkanen, S. Raman, At. Data Nucl. Data<br />

Tables 81 (2002) 1. [2] T. Kibédi, T.W. Burrows, M.B. Trzhaskovskaya, P.M. Davidson, C.W. Nestor, Jr.,<br />

Nucl. Instr. Meth. in Phys. Res. A 589 (2008) 202. [3] T. Kibédi, M.B. Trzhaskovskaya, M. Gupta, A.E.<br />

Stuchbery, At. Data Nucl. Data Tables 98 (2012) 313. [4] G. Gosselin, P. Morel, Phys. Rev. C 70 (2004)<br />

064603. [5] H.C. Pauli, U. Raff, Comp. Phys. Comm. 9 (1975) 392.<br />

LE 3 4:20 PM<br />

Survey and Evaluation of the Isobaric Analog States<br />

Marion Mac Cormick<br />

Institut de Physique Nucléaire, Orsay, CNRS/Université Paris Sud, 91406 Orsay CEDEX, FRANCE<br />

Georges Audi<br />

CSNSM, CNRS/Université Paris Sud, Bâtiment 108, 91405 Orsay Campus, FRANCE<br />

Aaldert H. Wapstra ∗<br />

NIKHEF, 1009DB Amsterdam, The Netherlands<br />

Isobaric analogue states (IAS) can be used to estimate the mass of nuclei belonging to isobars of the same<br />

isospin multiplet set. The Atomic Mass Evaluation (AME) had previously evaluated the experimental<br />

data used to establish the mass of these states. These masses were also used to establish a semi-empirical<br />

relationship between the members of any given mass multiplet via the isobaric mass multiplet equation,<br />

IMME. The experimental and IMME estimated IAS data have not been published in the AME since 1993<br />

[1]. However, given the recognized importance of isobaric states, it has been decided to reactivate these<br />

IAS studies, initially instigated by Aaldert H. Wapstra. In this conference we describe the reaction data<br />

used to establish the IAS. Cases where reaction data provide a better mass precision as compared to decay<br />

data will be presented. The particular cases of N=Z, T=1 ground states, and fragmented states will also<br />

be discussed. This work is an extension and update of the work carried out by Aaldert H. Wapstra until<br />

2003.<br />

[1] G. Audi, A.H. Wapstra and M. Dedieu, Nucl. Phys. A565(1993) 193-397. ∗ Deceased December 2006.<br />

LE 4 4:40 PM<br />

Systematics of Evaluated Double-Beta Decay Half-Life Times<br />

B. Pritychenko<br />

<strong>National</strong> Nuclear Data Center, <strong>Brookhaven</strong> <strong>National</strong> <strong>Laboratory</strong>, Upton, NY 11973-5000, USA<br />

A new evaluation of ββ(2ν) half-life values and their systematic are presented. These recommended values<br />

extend the previous evaluation [1] and include analysis of all recent measurements. T 2ν<br />

1/2 ∼ 1/E8 systematic<br />

trend has been observed for 128,130 Te recommended values. Such trend indicates similarities for nuclear<br />

matrix elements in Te nuclei and was predicted for ββ(2ν)-decay mode [2,3]. Current results are compared<br />

with large-scale shell-model calculations and experimental works.<br />

[1] B. Pritychenko, arXiv:1004.3280v1 [nucl-th] 19 Apr 2010. [2] B. Pontecorvo, Phys. Lett. B 26, 630<br />

(1968). [3] H. Primakoff and S.P. Rosen, Phys. Rev. 184, 1925 (1969).<br />

181

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