Search results for "octupole"

showing 4 items of 4 documents

Evidence of octupole-phonons at high spin in 207Pb

2019

A lifetime measurement of the 19/2 state in Pb has been performed using the Recoil Distance Doppler-Shift (RDDS) method. The nuclei of interest were produced in multi-nucleon transfer reactions induced by a Pb beam impinging on a Mo enriched target. The beam-like nuclei were detected and identified in terms of their atomic mass number in the VAMOS++ spectrometer while the prompt γ rays were detected by the AGATA tracking array. The measured large reduced transition probability B(E3,19/2→13/2)=40(8) W.u. is the first indication of the octupole phonon at high spin in Pb. An analysis in terms of a particle-octupole-vibration coupling model indicates that the measured B(E3) value in Pb is compa…

Nuclear and High Energy PhysicsPlunger devicePhononNuclear TheoryOctupole phonon[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]gamma-Ray trackingγ -Ray tracking01 natural sciences7. Clean energyRecoilVAMOS++ spectrometerAGATA spectrometer; Nuclear deformation; Octupole phonon; Plunger device; VAMOS++ spectrometer; γ-Ray tracking0103 physical sciencesPhysics::Atomic PhysicsAGATA spectrometerNuclear Experiment010306 general physicsSpin (physics)PhysicsVAMOS plus plus spectrometer010308 nuclear & particles physicsγ-Ray trackinglcsh:QC1-999Nuclear deformationAtomic physicslcsh:Physics
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Precision measurement of the magnetic octupole moment in 45Sc as a test for state-of-the-art atomic- and nuclear-structure theory

2020

We report on measurements of the hyperfine $A, B$ and $C$-constants of the $3d4s^2 ~^2D_{5/2}$ and $3d4s^2 ~^2D_{3/2}$ atomic states in $^{45}$Sc. High-precision atomic calculations of the hyperfine fields of these states and second-order corrections are performed, and are used to extract $C_{5/2}=-0.06(6)$ kHz and $C_{3/2}=+0.04(3)$ kHz from the data. These results are one order of magnitude more precise than the available literature. From the combined analysis of both atomic states, we infer the nuclear magnetic octupole moment $\Omega = -0.07(53) \mu_N b$, including experimental and atomic structure-related uncertainties. With a single valence proton outside of a magic calcium core, scan…

Nuclear and High Energy PhysicsoctupoleNuclear Theorynuclear density functional theory010308 nuclear & particles physicsPhysicsQC1-999tiheysfunktionaaliteoriaFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)0103 physical sciencesnuclear structurePhysics::Atomic Physicsoktupooli ydinrakenneNuclear Experiment (nucl-ex)010306 general physicsydinfysiikkaNuclear Experiment
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Backbending in the pear-shaped 223(90)Th nucleus: Evidence of a high-spin octupole to quadrupole shape transition in the actinides

2017

International audience; Relatively neutron-rich thorium isotopes lie at the heart of a nuclear region of nuclei exhibiting octupole correlation effects. The detailed level structure of Th223 has been investigated in measurements of γ radiation following the fusion-evaporation channel of the Pb208(O18,3n)Th223 reaction at 85 MeV beam energy. The level structure has been extended up to spin 49/2, and 33 new γ rays have been added using triple-γ coincidence data. The spins and parities of the newly observed states have been confirmed by angular distribution ratios. In addition to the two known yrast bands based on a K=5/2 configuration, a non-yrast band has been established up to spin 35/2. We…

octupole correlationNuclear Theorytoriumpear-shaped nuclei[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment
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Identification of the Jπ = 1− state in 218Ra populated via α decay of 222Th

2016

The α decay of 222Th populating the low-lying J π = 3− state, and also a proposed 1− state, in 218Ra has been observed. The observations suggest an excitation energy of 853 keV for the 1− state, which is 60 keV above the 3− state. The hindrance factors of these α decays give a possible boundary to the region of ground-state octupole deformation in the light-actinide nuclei. The relative positions of the J π = 1− and 3− states suggest they are produced by an octupole-vibrational mechanism, as opposed to α clustering or rotations of a reflection-asymmetric octupole-deformed shape. peerReviewed

radiumNuclear Theoryoctupole correlationsdeformed nucleitoriumexcited states
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