Measurements on prototype Ge and BGO detectors for the Eurogam array
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Anti-Compton shield for COMPEX germanium detector modules
2023, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentExperimental observation of the M1 scissors mode in <sup>254</sup>No
2022, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsCitation Excerpt :The 254No ions were separated in flight in the gas-filled recoil separator RITU [24,25], and implanted in a pair of double-sided silicon strip detectors (DSSDs) placed at the focal plane of RITU. Prompt γ rays were detected by the Jurogam II germanium-detector array [26], consisting of 15 Compton-suppressed coaxial detectors [27,28] and 24 clover-type detectors [29]. The prompt γ rays were selected in delayed coincidence with recoils detected in the DSSDs.
Evidence against the wobbling nature of low-spin bands in <sup>135</sup>Pr
2022, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsLifetime measurements of excited states in <sup>169,171,173</sup>Os: Persistence of anomalous B(E2) ratios in transitional rare earth nuclei in the presence of a decoupled i<inf>13/2</inf> valence neutron
2021, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsCitation Excerpt :Prompt γ rays at the target position were detected by the JUROGAM II germanium detector array consisting of 15 Eurogam Phase I-type [21] and 24 Euroball clover [22] escape-suppressed detectors, with a total photopeak efficiency of ∼6% at 1.3 MeV.
Lifetime measurements of excited states in <sup>163</sup>W and the implications for the anomalous B(E2) ratios in transitional nuclei
2019, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsCitation Excerpt :The target-to-degrader distance, x, was changed to allow excited-state lifetimes to be measured using the recoil-distance Doppler-shift (RDDS) technique [3]. Gamma rays emitted at the target position were detected by the JUROGAM II γ-ray spectrometer comprising 15 Eurogam Phase 1-type [9] and 24 Eurogam clover [10] escape-suppressed hyperpure germanium detectors. The velocity-degraded fusion-evaporation residues were transported through the RITU gas-filled separator [11,12] and implanted into the double-sided silicon strip detectors (DSSDs) of the GREAT spectrometer located at the focal plane [13].
A time-of-flight correction procedure for fast-timing data of recoils with varying implantation positions at a spectrometer focal plane
2019, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment