2020
DOI: 10.1016/j.physletb.2019.135140
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Multi-quasiparticle sub-nanosecond isomers in 178W

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Cited by 14 publications
(10 citation statements)
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“…Due to the fact that the state of interest is below the long-lived 6 + isomer, we use delayed LaBr 3 (Ce) events in a similar way as described in Ref. [52]. A HPGe sum gate on the 1279 keV, 2 + 1 → 0 + 1 transition together with a prompt transition above the isomer is used to tag the 134 Te nucleus.…”
Section: B Remeasurement Of Half-lives In 134 Tementioning
confidence: 99%
“…Due to the fact that the state of interest is below the long-lived 6 + isomer, we use delayed LaBr 3 (Ce) events in a similar way as described in Ref. [52]. A HPGe sum gate on the 1279 keV, 2 + 1 → 0 + 1 transition together with a prompt transition above the isomer is used to tag the 134 Te nucleus.…”
Section: B Remeasurement Of Half-lives In 134 Tementioning
confidence: 99%
“…The desired reaction was via 164 Dy( 18 O, 16 O) 166 Dy. The production of this channel was significantly suppressed relative to the main reaction channels (with cross sections approximately 10 3 times stronger than the 2n transfer) from the Coulomb excitation by inelastic scattering on the 164 Dy target nucleus, and the 164 Dy( 18 O, 4n) 178 W fusion evaporation reaction (a more detailed study of 178 W from this experiment can be found in [18]).…”
Section: Experimental Details and Reaction Channel Selectionmentioning
confidence: 92%
“…The states of interest in 166 Dy were populated at an experiment carried out using the accelerator at the ALTO facility at the IPN Orsay. A pulsed 18 O beam was provided at three separate primary energies of 71, 76, and 80 MeV, each with a pulse duration of 2 ns and a period of 400 ns, and an average current of 35 enA charge state Q = 6 + . A 164 Dy target of 6.3 mg/cm 2 and 95% isotopic enrichment was used with 1 mg/cm 2 Au backing.…”
Section: Experimental Details and Reaction Channel Selectionmentioning
confidence: 99%
“…[9] and already used in Refs. [10,11,12]. The lifetime value was obtained by 2τ = ∆C-PRD(E f ,E d ), where ∆C is the centroid difference between the delayed (D) and antidelayed (AD) time distributions.…”
Section: The Experimentsmentioning
confidence: 99%