0000000000240055

AUTHOR

J. A. Cameron

showing 5 related works from this author

Evidence for isovector neutron-proton pairing from high-spin states inN=Z74Rb

2003

High-spin states in the odd-odd N=Z nucleus Rb-74(37)37 were studied using the Ca-40(Ca-40,alphanp) reaction. A previously observed odd-spin T=0 band has been extended to I-pi=(31(+)) and an even-spin T=0 band has been observed for the first time to I-pi=(22(+)); both have a pi(g(9/2))circle timesnu(g(9/2)) structure. A strongly coupled low-spin T=0,K=3 band has been interpreted as being based upon a pi[312]3/2 circle timesnu[312]3/2 configuration. Cranked relativistic Hartree-Bogoliubov calculations, which are corrected for the t=1 np-pair field by restoring isospin symmetry, reproduce the observed spectrum. These new results provide evidence for the existence of an isovector pair field th…

PhysicsNuclear and High Energy PhysicsIsovectorProtonSpin statesField (physics)IsospinPairingNuclear TheoryNeutronAtomic physicsSymmetry (physics)Physical Review C
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Evidence for Magnetic Rotation in the Light Tin Region

2000

Lifetimes have been measured for three M1 bands in light Sn/Cd nuclei using the DSAM technique. B(M1) values deduced from these measurements show a rapid decrease with increasing spin for a given configuration. The results have been compared with both Tilted axis cranking and semi-empirical model calculations. These suggest that the shears mechanism is present in this mass region, and that the band in 106Sn appears to be the first example of almost pure magnetic rotation.

PhysicschemistryMagnetic rotationchemistry.chemical_elementAtomic physicsCondensed Matter PhysicsSpin (physics)TinMathematical PhysicsAtomic and Molecular Physics and OpticsPhysica Scripta
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Mirror symmetry at high spin in51Feand51Mn

2000

Gamma decays from excited states in the ${T}_{z}=\ensuremath{-}\frac{1}{2}$ nucleus ${}^{51}$Fe have been observed for the first time. The differences in excitation energies as compared with those of the mirror partner, ${}^{51}$Mn, have been interpreted in terms of Coulomb effects and the resulting Coulomb energy differences (CED) can be understood intuitively in terms of particle-alignment effects. A new CED effect has been observed, in which different CED trends have been measured for each signature of the rotational structures that characterize these mid-${f}_{7/2}$ shell nuclei. Large-scale $\mathrm{fp}$-shell model calculations have been used to compute the trends of the CED as a func…

PhysicsNuclear and High Energy PhysicsExcited stateElectric potential energyGamma rayCoulombAtomic physicsMirror symmetrySymmetry (physics)ExcitationSpin-½Physical Review C
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Anomalous Coulomb matrix elements in thef7/2shell

2003

γ decays from high-spin states in the N=Z-1 nucleus 2753Co26 have been identified for the first time. Level energies and Coulomb energy differences between these states and their analogs in its mirror nucleus 53Fe have been compared with large-scale pf shell-model calculations, which offer excellent agreement. New information has been obtained on two-proton Coulomb matrix elements needed in the interpretation. These have been extracted from the data via a number of methods and are shown to exhibit an anomalous behavior for the J=2 coupling.

CouplingPhysicsNuclear and High Energy PhysicsMatrix (mathematics)medicine.anatomical_structureElectric potential energyCoulombShell (structure)medicineAnomalous behaviorAtomic physicsNucleusInterpretation (model theory)Physical Review C
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Application of ultra-fast timing techniques to the study of exotic and weakly produced nuclei

2005

Ultra-fast time-delayed techniques have been recently applied in a number of studies where exotic nuclei were identified using advanced selection techniques. These include large Compton-suppressed Ge arrays, in-flight separators or recoil separators. Some of the new results are discussed in this presentation. Besides the results for $^{32}$Mg and $^{96}$Pd, they include the first determination of the half-life of the $8^+$ state in $^{80}$Ge, $T_1/2$ = 2.95(6) ns, and significantly more precise results for $^{51}$Mn (3680 keV level) and $^{48}$V (421 keV level), $T_1/2$ = 1760(40) ps and $T_1/2$ $\leq$ 135 ps, respectively. Development of new scintillators will steadily improve precision an…

PhysicsNuclear physicsNuclear and High Energy Physics010308 nuclear & particles physics0103 physical sciencesHardware_INTEGRATEDCIRCUITSUltra fastStatistical physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]010306 general physics7. Clean energy01 natural sciencesSelection (genetic algorithm)
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