Negative-Parity States in 196Pt

Cizewski, J. A.; Casten, R. F.; Macphail, M.R.; Smith, Gregory J.; Stelts, M.L.; Kane, W.R.; Börner, H. G.; Davidson, W.F.

doi:10.1007/978-1-4613-2940-4_47

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1979

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“…3 H = To S+S +~2Di; +;~hr Pr"P"r, The integer k is the same as mentioned in (6). The multipole operator of zero rank is just the fermion valence number operator po=n (9C) tt'!i and, for the states within the (S ,D ) space , the dipole operator is proportional to the angular momentum operator.…”

Section: Discussionmentioning

confidence: 99%

Fermion Hamiltonians with Monopole and Quadrupole Pairing

Ginocchio

1979

Interacting Bosons in Nuclear Physics

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Ely ncceptmnce of this article for pualIcLtion, the publisher recognizes the Government'~(licenselright# in unycopyright undthefkwernment andit~authorir.ed representatives haw unrestricted right to reproduce in whol~or In purt mld article under any copyright nccured by the publi:l%er. The Los Alnmo~Scientific Luborntov requeutsthat the publisher identify this article as work performed under thenuspicesof the [JSHR[)A.

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Section: Discussionmentioning

confidence: 99%

Fermion Hamiltonians with Monopole and Quadrupole Pairing

Ginocchio

1979

Interacting Bosons in Nuclear Physics

View full text Add to dashboard Cite

show abstract

Negative-Parity States in 196Pt

Cited by 1 publication

References 6 publications

Fermion Hamiltonians with Monopole and Quadrupole Pairing

Fermion Hamiltonians with Monopole and Quadrupole Pairing

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