2017
DOI: 10.1103/physrevc.95.054319
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Abrupt shape transition at neutron number N=60 : B(E2) values in Sr

Abstract: Lifetimes of low-lying yrast states in neutron-rich 94,96,98 Sr have been measured by Germanium-gated γ -γ fast timing with LaBr3(Ce) detectors using the EXILL&FATIMA spectrometer at the Institut Laue-Langevin. Sr fission products were generated using cold-neutron-induced fission of 235 U and stopped almost instantaneously within the thick target. The experimental B(E2) values are compared with results of Monte Carlo shell-model calculations made without truncation on the occupation numbers of the orbits span… Show more

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Cited by 34 publications
(29 citation statements)
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“…The lifetime of the 121.7-keV level has been reported to be measured several times [31] and, therefore, constitutes a good test case. Furthermore several lifetimes measured from this data set have been reported previously [32][33][34]. The 192.6-536.0-121.7-keV cascade was used for this.…”
Section: Resultsmentioning
confidence: 99%
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“…The lifetime of the 121.7-keV level has been reported to be measured several times [31] and, therefore, constitutes a good test case. Furthermore several lifetimes measured from this data set have been reported previously [32][33][34]. The 192.6-536.0-121.7-keV cascade was used for this.…”
Section: Resultsmentioning
confidence: 99%
“…A thorough description of this method is presented in Refs. [33,34] Transition branching ratios from [31] and corrections for internal conversion [37] were used to convert the measured level lifetimes into partial stretched E 2 lifetimes (τ E 2 ). Reduced transition rates were then calculated using the formula…”
Section: -mentioning
confidence: 99%
“…As the subscript "FEP" indicates, this only holds for events where no time-correlated background is present. An analytical background time correction is used to interpolate the time-correlated background at the energy of interest, which has been shown to be most reliable [2,[28][29][30]:…”
Section: Fast-timing Methodsmentioning
confidence: 99%
“…The product of the strength constant ν times the boson quadrupole operator for proton bosonsQ (2) π times the quadrupole operator for the odd neutronq (2) ν represents the quadrupole dynamical term [41]. The second term describes the exchange interaction introduced to consider that the bosons are in fact nucleon pairs.…”
Section: -5mentioning
confidence: 99%
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