1991
DOI: 10.1016/0375-9474(91)90001-m
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Retardation of B(E2; 01+ → 21+) rates in 90–96Sr and strong subshell closure effects in the A ~ 100 region

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Cited by 153 publications
(51 citation statements)
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“…We have investigated experimentally the β − decay of 66 Co to 66 Ni with the aim of measuring the half-life of the excited states populated in 66 Ni by means of the the Advanced Time-Delayed βγγ(t) method described in [20][21][22]. This experiment was part of a wider campaign to study the evolution of collectivity below 68 Ni [23][24][25].…”
Section: Fig 2 (Color Online) (Left)mentioning
confidence: 99%
“…We have investigated experimentally the β − decay of 66 Co to 66 Ni with the aim of measuring the half-life of the excited states populated in 66 Ni by means of the the Advanced Time-Delayed βγγ(t) method described in [20][21][22]. This experiment was part of a wider campaign to study the evolution of collectivity below 68 Ni [23][24][25].…”
Section: Fig 2 (Color Online) (Left)mentioning
confidence: 99%
“…The experimental setup and data collection were optimized for the application of the ATD βγ γ (t) method described in [15,16,19], thus only a few details are given below. A time-delayed βγ (t) coincidence system was set between the β detector and each of the γ detectors and thus three parameters were required per coincident βγ (t) event: the energies of the β particle and the γ ray, and the time-delay between the β and γ events.…”
Section: Technical Aspectsmentioning
confidence: 99%
“…This calibration was further verified using the most intense γ lines in 30 Si from the experiment. In the ATD method [15,16,19] the time responses of the fast-timing γ detectors (BaF 2 crystals with a FWHM time resolution around 100 ps at 1 MeV) are carefully calibrated (to a picosecond precision) for various types of interactions of γ rays in the crystal (Compton and full energy peak (FEP) events). It is also checked that the shape of time spectra for prompt radiation is close to symmetric quasi-Gaussians over the range of the γ -ray energies of interest.…”
Section: Technical Aspectsmentioning
confidence: 99%
“…The ATD method was invented by Henryk Mach in 1986 in the TRISTAN facility located at Brookhaven National Laboratory, and developed and published by Mach et al [6][7][8]. As other delayed coincidence methods, it is based in the time distribution between the population of an excited state and its de-excitation.…”
Section: The Advanced Time Delayed βγγ(T) Method-technical Detailsmentioning
confidence: 99%