0000000000863140

AUTHOR

J. Lintott

showing 2 related works from this author

Electromagnetic transition rates in theN=80nucleus58138Ce

2013

The half-life of the Iπ=6+ yrast state at Ex=2294 keV in 138Ce has been measured as T1/2=880(19) ps using the fast-timing γ-ray coincidence method with a mixed LaBr3(Ce)-HPGe array. The excited states in 138Ce have been populated by the 130Te(12C,4n) fusion-evaporation reaction at an incident beam energy of 56 MeV. The extracted B(E2;61+→41+)=0.101(24) W.u. value is compared with the predictions of truncated basis shell model calculations and with the systematics of the region. This shows an anomalous behavior compared to the neighboring isotonic and isotopic chains. Half-lives for the yrast 5-, 11+ and 14+ states in 138Ce have also been determined in this work.

PhysicsNuclear and High Energy PhysicsWork (thermodynamics)medicine.anatomical_structureYrastExcited stateSHELL modelmedicineIncident beamAnomalous behaviorAtomic physicsNucleusCoincidencePhysical Review C
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Electromagnetic Transition Rate Measurements in theN=80 Isotone,138Ce

2012

A study of intrinsic state halflife measurements in the N=80 nucleus 138Ce has been made using the 130Te(12C,4n)138Ce fusion evaporation reaction at beam energy of 56 MeV. The fast-timing gamma-ray coincidence method was used with a mixed LaBr3(Ce)-HPGe array to establish the lifetimes of the yrast 6+ state at 2294 keV, the Iπ=5− state at 2218 keV, the Iπ=11+ state at 3943 keV and the 14+ state at that at 5312 keV, all of which are in the sub nanosecond regime. Reduced transition probabilities have been calculated for the electromagnetic decays from these states.

PhysicsHistoryFusionAstrophysics::High Energy Astrophysical PhenomenaIsotoneYrastEvaporationState (functional analysis)NanosecondTransition rate matrixCoincidenceComputer Science ApplicationsEducationNuclear physicsAtomic physicsNuclear ExperimentJournal of Physics: Conference Series
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