PaperPanorama

Nuclear Theory·nucl-th

Monday·May 9, 2016

5 papers2 primary·3 cross-listed

  1. 01

    [Submitted on 6 May 2016]

    Quantal rotation and its coupling to intrinsic motion in nuclei

    Takashi Nakatsukasa (1 and 2) · Kenichi Matsuyanagi (2 and 3) · Masayuki Matsuzaki (4) · Yoshifumi R. Shimizu (5) ((1) University of Tsukuba, (2) RIKEN Nishina Center, (3) YITP, (4) Fukuoka University of Education, (5) Kyushu University)

    Symmetry breaking is an importance concept in nuclear physics and other fields of physics. Self-consistent coupling between the mean-field potential and the single-particle motion is a key ingredient in the unified model of Bohr and Mottelson, which could lead to a deformed nucleus as a consequence of spontaneous breaking of the rotational symmetry. Some remarks on the finite-size quantum effects are given. In finite nuclei, the deformation inevitably introduces the rotation as a symmetry-restoring collective motion (Anderson-Nambu-Goldstone mode), and the rotation affects the intrinsic motion. In order to investigate the interplay between the rotational and intrinsic motions in a variety of collective phenomena, we use the cranking prescription together with the quasiparticle random phase approximation. At low spin, the coupling effect can be seen in the generalized intensity relation. A feasible quantization of the cranking model is presented, which provides a microscopic approach to the higher-order intensity relation. At high spin, the semiclassical cranking prescription works well. We discuss properties of collective vibrational motions under rapid rotation and/or large deformation. The superdeformed shell structure plays a key role in emergence of a new soft mode which could lead to instability toward the octupole shape. A wobbling mode of excitation, which is a clear signature of the triviality, is discussed in terms of a microscopic point of view. A crucial role played by the quasiparticle alignment is presented.

    Comments:
    38 pages, 11 figures, Contribution to the Focus issue to celebrate the 40 year anniversary of the 1975 Nobel Prize
    Subjects:
    Nuclear Theory (nucl-th)
    arXiv:
    1605.01876 [pdf]
    Phys.Scripta(2016)·19 citations
  2. 02

    [Submitted on 6 May 2016]

    Role of the total isospin 3/2 component in three-nucleon reactions

    H. Witała · J. Golak · R. Skibiński · K. Topolnicki · E. Epelbaum · K. Hebeler · H. Kamada · H. Krebs · U.-G. Meißner · A. Nogga

    We discuss the role of the three-nucleon isospin T=3/2 amplitude in elastic neutron-deuteron scattering and in the deuteron breakup reaction. The contribution of this amplitude originates from charge-independence breaking of the nucleon-nucleon potential and is driven by the difference between neutron-neutron (proton-proton) and neutron-proton forces. We study the magnitude of that contribution to the elastic scattering and breakup observables, taking the locally regularized chiral N4LO nucleon-nucleon potential supplemented by the chiral N2LO three-nucleon force. For comparison we employ also the Av18 nucleon-nucleon potential combined with the Urbana IX three-nucleon force. We find that the isospin T=3/2 component is important for the breakup reaction and the proper treatment of charge-independence breaking in this case requires the inclusion of the 1S0 state with isospin T=3/2. For neutron-deuteron elastic scattering the T=3/2 contributions are insignificant and charge-independence breaking can be accounted for by using the effective t-matrix generated with the so-called "2/3-1/3" rule.

    Comments:
    24 pages, 8 figures, 3 Tables
    Subjects:
    Nuclear Theory (nucl-th)
    arXiv:
    1605.02011 [pdf]
    Few Body Syst.(2016)·14 citations

Affiliations

first authorsco-authorsvia INSPIRE