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Narrowing of the neutron sd–pf shell gap in 29Na

Authors :
G. A. Demand
R. Churchman
A. A. Phillips
J. Wong
A. M. Hurst
K. L. Green
W. D. Kulp
C. J. Pearson
S. Triambak
P. M. Walker
L. Nelson
D. S. Cross
R. Maharaj
A. J. Boston
H. C. Boston
Ching-Yen Wu
C Gray-Jones
J. L. Wood
D. Bandyopadhyay
Chandana Sumithrarachchi
S. Mythili
C. J. Barton
R. A. E. Austin
M. A. Stoyer
P. E. Garrett
A. B. Hayes
Susan Rigby
G. Lee
S. J. Williams
M. Djongolov
Elizabeth Padilla-Rodal
B. A. Millar
K. G. Leach
T.E. Drake
G. Hackman
M. Porter-Peden
D. C. Oxley
Stephen Lloyd
Fred Sarazin
C. E. Svensson
G. C. Ball
S. Colosimo
A. N. Grint
M. A. Schumaker
J. P. Martin
J. A. Becker
D. Cline
P. J. Nolan
Source :
Physics Letters B. 674:168-171
Publication Year :
2009
Publisher :
Elsevier BV, 2009.

Abstract

The wave-function composition for the low-lying states in 29 Na was explored by measuring their electromagnetic properties using the Coulomb-excitation technique. A beam of 29 Na ions, postaccelerated to 70 MeV, bombarded a 110 Pd target with a rate of up to 600 particles per second at the recently commissioned ISAC-II facility at TRIUMF. Six segmented HPGe clover detectors of the TIGRESS γ -ray spectrometer were used to detect deexcitation γ rays in coincidence with scattered or recoiling charged particles in the segmented silicon detector, BAMBINO. The reduced transition matrix element | 〈 5 2 1 + | | E 2 | | 3 2 gs + 〉 | in 29 Na was derived to be 0.237(21) e b from the measured γ -ray yields for both projectile and target. This first-time measured value is consistent with the most recent Monte Carlo shell-model calculation, indicating a significant admixture of both sd and pf components in the wave function, and also providing evidence for the narrowing of the neutron s d – p f shell gap from ∼ 6 MeV for stable nuclei to ∼ 3 MeV for 29 Na.

Details

ISSN :
03702693
Volume :
674
Database :
OpenAIRE
Journal :
Physics Letters B
Accession number :
edsair.doi.dedup.....86e48471abbcbc682dc35c211f21ab9a