1992
DOI: 10.1103/physrevc.46.541
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Intruder analog states: New classification of particle-hole excitations near closed shells

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Cited by 57 publications
(32 citation statements)
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“…On the basis of intruder spin symmetry [25,26], no distinction is made between particle and hole bosons. Hence, the shell-model space that includes 0p-0h, 2p-2h, and 4p-4h shell-model excitations corresponds to a [N ] ⊕ [N + 2] ⊕ [N + 4] boson space.…”
Section: The Formalismmentioning
confidence: 99%
“…On the basis of intruder spin symmetry [25,26], no distinction is made between particle and hole bosons. Hence, the shell-model space that includes 0p-0h, 2p-2h, and 4p-4h shell-model excitations corresponds to a [N ] ⊕ [N + 2] ⊕ [N + 4] boson space.…”
Section: The Formalismmentioning
confidence: 99%
“…Neutron-deficient lead isotopes present a nice example of the shape coexistence phenomena [2]: In the 186,188 Pb nuclei, the presence of three low-lying 0 + states and other additional experimental data strongly suggests the coexistence of spherical, prolate, and oblate shapes. In the context of the nuclear shell model [6][7][8][9], the emergence of low-lying excited 0 + states is traced back to the proton particle-hole excitation across the Z = 82 closed shell. The residual interaction between protons and neutrons is enhanced due to this cross-shell excitation, resulting in the lowering of the excited 0 + states.…”
Section: Introductionmentioning
confidence: 99%
“…The energy spectrum remains remarkably constant in the mass interval 178 ≤ A ≤ 186, contrasting with a different structure that shows a number of up sloping levels with increasing mass number A beyond mass A = 186. excitations [29]. On the basis of intruder spin symmetry [33,73], no distinction is made between particle and hole bosons. Hence, the model space which includes the regular proton 4h configurations and a number of valence neutrons outside of the N = 82 closed shell (corresponding to the standard IBM treatment for the Pt even-even nuclei) as well as the proton 6h-2p configurations and the same number of valence neutrons corresponds to a [N] ⊕ [N + 2] boson space (N, being the number of active protons, counting both, proton holes and particles, plus the number of valence neutrons outside the N = 126 or the N = 82 closed shell (depending on the nearest closed shell), divided by 2 as the boson number).…”
Section: The Experimental Data In the Even-even Pt Nucleimentioning
confidence: 99%