TY - JOUR
T1 - Low-spin mixed particle-hole structures in 185W
AU - Bondarenko, V.
AU - Honzátko, J.
AU - Tomandl, I.
AU - von Egidy, T.
AU - Wirth, H. F.
AU - Sukhovoj, A. M.
AU - Malov, L. A.
AU - Simonova, L. I.
AU - Alexa, P.
AU - Berziņš, J.
AU - Hertenberger, R.
AU - Eisermann, Y.
AU - Graw, G.
N1 - Funding Information:
We are grateful to P. Maier-Komor and to K. Nacke for the target preparation and to T. Faester-mann for the Q3D maintenance. The technical staffs of the reactor at Rˇ ež and of the accelerator laboratory in Munich deserve appreciation for providing us with excellent beams. J.B. and V.B. are very appreciative to the TU München for the hospitality. One of us (V.B.) is grateful also to the NPI, Rˇ ež, for the hospitality and helpful cooperation and discussions. This work was supported by the Grant Agency of the Czech Republic (Nos. 202/03/0891, 202/99/D087) and by the Volkswagen Foundation, Hannover, and the Deutsche Forschungsgemeinschaft, Bonn (Eg 25/4).
PY - 2005/12/12
Y1 - 2005/12/12
N2 - The level structure of 185W has been studied using the prompt and delayed gamma-gamma coincidences from thermal neutron capture in 184W accompanied with the one-nucleon transfer reactions (d, p) and (d, t) with polarized beams. From these data and those of previous studies a total of 183 levels has been established for energies below 3 MeV. Many of these states have been grouped into rotational bands built on 28 intrinsic states of quasiparticle and quasiparticle-plus-phonon character. Although the DWBA analysis permitted definite spin-parity assignments for most of states a large number of particle transitions have 'anomalous' angular and asymmetry shapes with respect to the DWBA which indicate an influence of strong mixing between particle and hole states. The extra exchange of phonons and the significance of configurational ΔN = plusmn;2 mixing across the Fermi surface lead to a fine structure in the fragmentation of most single-particle strengths and at the same time has the effect of breakdown of the individual properties of Nilsson states. The accumulated l = 1 (d, p) sum is about a factor two smaller than the equivalent (d, t) strength. Thus, the previously observed loss of the (d, p) strength in the W nuclei with A = 184, 185 is presumably because of their redistribution amongst particle- and hole-type states. The observed states below 2 MeV are compared with predictions of the quasiparticle-phonon nuclear model.
AB - The level structure of 185W has been studied using the prompt and delayed gamma-gamma coincidences from thermal neutron capture in 184W accompanied with the one-nucleon transfer reactions (d, p) and (d, t) with polarized beams. From these data and those of previous studies a total of 183 levels has been established for energies below 3 MeV. Many of these states have been grouped into rotational bands built on 28 intrinsic states of quasiparticle and quasiparticle-plus-phonon character. Although the DWBA analysis permitted definite spin-parity assignments for most of states a large number of particle transitions have 'anomalous' angular and asymmetry shapes with respect to the DWBA which indicate an influence of strong mixing between particle and hole states. The extra exchange of phonons and the significance of configurational ΔN = plusmn;2 mixing across the Fermi surface lead to a fine structure in the fragmentation of most single-particle strengths and at the same time has the effect of breakdown of the individual properties of Nilsson states. The accumulated l = 1 (d, p) sum is about a factor two smaller than the equivalent (d, t) strength. Thus, the previously observed loss of the (d, p) strength in the W nuclei with A = 184, 185 is presumably because of their redistribution amongst particle- and hole-type states. The observed states below 2 MeV are compared with predictions of the quasiparticle-phonon nuclear model.
KW - DWBA analysis
KW - E, I, γγ-coincidences
KW - Enriched targets
KW - Ge detectors
KW - Measured particle spectra, σ(θ), asymmetry
KW - Measured prompt and delayed
KW - Nuclear reactions
KW - Q3D magnetic spectrograph
KW - QPNM calculation and comparison
KW - W deduced levels, J, π, γ-branching ratios, cross sections, binding energy, spectroscopic factors
KW - W(n, γ), E=thermal
KW - W(polarized d,p), E = 18,21 MeV
KW - W(polarized d,t) E = 22 MeV
UR - http://www.scopus.com/inward/record.url?scp=27744595938&partnerID=8YFLogxK
U2 - 10.1016/j.nuclphysa.2005.08.003
DO - 10.1016/j.nuclphysa.2005.08.003
M3 - Article
AN - SCOPUS:27744595938
SN - 0375-9474
VL - 762
SP - 167
EP - 215
JO - Nuclear Physics, Section A
JF - Nuclear Physics, Section A
IS - 3-4
ER -