6533b824fe1ef96bd127fdef

RESEARCH PRODUCT

Kπ=8−isomers andKπ=2−octupole vibrations inN=150shell-stabilized isotones

C. J. ListerJohn P. GreeneD. SeweryniakS. K. TandelF. G. KondevS. ZhuB. B. BackP. ChowdhuryT. L. KhooT. LauritsenS. GrosR.-d. HerzbergD. PetersonS. EeckhaudtG. D. JonesJ. QianA. RobinsonAndreas Martin HeinzU. S. TandelXuan WangXuan WangI. AhmadPaul GreenleesR. V. F. JanssensM. AsaiC. N. DavidsM. P. CarpenterTakashi Nakatsukasa

subject

PhysicsNuclear and High Energy PhysicsMean field theoryProtonQuasiparticleWoods–Saxon potentialAtomic numberAtomic physicsQuantum numberRandom phase approximationEnergy (signal processing)

description

Isomers have been populated in {sup 246}Cm and {sup 252}No with quantum numbers K{sup {pi}}=8{sup -}, which decay through K{sup {pi}}=2{sup -} rotational bands built on octupole vibrational states. For N=150 isotones with (even) atomic number Z=94-102, the K{sup {pi}}=8{sup -} and 2{sup -} states have remarkably stable energies, indicating neutron excitations. An exception is a singular minimum in the 2{sup -} energy at Z=98, due to the additional role of proton configurations. The nearly constant energies, in isotones spanning an 18% increase in Coulomb energy near the Coulomb limit, provide a test for theory. The two-quasiparticle K{sup {pi}}=8{sup -} energies are described with single-particle energies given by the Woods-Saxon potential and the K{sup {pi}}=2{sup -} vibrational energies by quasiparticle random-phase approximation calculations. Ramifications for self-consistent mean-field theory are discussed.

https://doi.org/10.1103/physrevc.78.034308