Abstract
Analogous to the equivalence between the SU(6) quadrupole-phonon model (TQM) and the interacting boson model (IBM), the equivalence is pointed out for odd systems between the SU(6) particle quadrupole-phonon coupling model (PTQM) and the interacting boson-fermion model (IBFM). PTQM is formulated starting from the Dyson representation for the odd system. Different aspects of the SU(3) limit of TQM and PTQM are studied; the quadrupole-phonon block structure of rotational bands in even and odd nuclei and analytic expressions based on the coherent state; signature effects generated in PTQM; electromagnetic properties and correction factors for PTQM; overlaps of the PTQM analogs of Nilsson states with Coriolis-coupled Nilsson states and the relation to the rotational model representation.
Paar, V;
Brant, S;
[1]
Canto, L F;
[2]
Leander, G;
[3]
Oak Ridge National Lab., TN (USA));
Vouk, M
[4]
- Zagreb Univ. (Yugoslavia). Prirodoslovno Matematicki Fakultet
- Rio de Janeiro Univ. (Brazil). Inst. de Fisica
- Lund Inst. of Tech. (Sweden). Dept. of Mathematical Physics
- Zagreb Univ. (Yugoslavia). Computing Centre SRCE
Citation Formats
Paar, V, Brant, S, Canto, L F, Leander, G, Oak Ridge National Lab., TN (USA)), and Vouk, M.
SU(6) quadrupole phonon model for even and odd nuclei and the SU(3) limit.
Netherlands: N. p.,
1982.
Web.
Paar, V, Brant, S, Canto, L F, Leander, G, Oak Ridge National Lab., TN (USA)), & Vouk, M.
SU(6) quadrupole phonon model for even and odd nuclei and the SU(3) limit.
Netherlands.
Paar, V, Brant, S, Canto, L F, Leander, G, Oak Ridge National Lab., TN (USA)), and Vouk, M.
1982.
"SU(6) quadrupole phonon model for even and odd nuclei and the SU(3) limit."
Netherlands.
@misc{etde_5227020,
title = {SU(6) quadrupole phonon model for even and odd nuclei and the SU(3) limit}
author = {Paar, V, Brant, S, Canto, L F, Leander, G, Oak Ridge National Lab., TN (USA)), and Vouk, M}
abstractNote = {Analogous to the equivalence between the SU(6) quadrupole-phonon model (TQM) and the interacting boson model (IBM), the equivalence is pointed out for odd systems between the SU(6) particle quadrupole-phonon coupling model (PTQM) and the interacting boson-fermion model (IBFM). PTQM is formulated starting from the Dyson representation for the odd system. Different aspects of the SU(3) limit of TQM and PTQM are studied; the quadrupole-phonon block structure of rotational bands in even and odd nuclei and analytic expressions based on the coherent state; signature effects generated in PTQM; electromagnetic properties and correction factors for PTQM; overlaps of the PTQM analogs of Nilsson states with Coriolis-coupled Nilsson states and the relation to the rotational model representation.}
journal = []
volume = {378:1}
journal type = {AC}
place = {Netherlands}
year = {1982}
month = {Apr}
}
title = {SU(6) quadrupole phonon model for even and odd nuclei and the SU(3) limit}
author = {Paar, V, Brant, S, Canto, L F, Leander, G, Oak Ridge National Lab., TN (USA)), and Vouk, M}
abstractNote = {Analogous to the equivalence between the SU(6) quadrupole-phonon model (TQM) and the interacting boson model (IBM), the equivalence is pointed out for odd systems between the SU(6) particle quadrupole-phonon coupling model (PTQM) and the interacting boson-fermion model (IBFM). PTQM is formulated starting from the Dyson representation for the odd system. Different aspects of the SU(3) limit of TQM and PTQM are studied; the quadrupole-phonon block structure of rotational bands in even and odd nuclei and analytic expressions based on the coherent state; signature effects generated in PTQM; electromagnetic properties and correction factors for PTQM; overlaps of the PTQM analogs of Nilsson states with Coriolis-coupled Nilsson states and the relation to the rotational model representation.}
journal = []
volume = {378:1}
journal type = {AC}
place = {Netherlands}
year = {1982}
month = {Apr}
}