Collective Motion of a pure Octupole Deformed System

  • The collective motion of a pure octupole deformed system is treated as the vibrations in body-fixed frame and rotation of this system about the axes of lab-system,as well as the coupling between vibrations and rotation. The quantized operator of kinetic energy is derived and the collective spectra built on some special equilibrium shape are discussed.
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  • [1] Bohr A,Dan. Mat. Fys. Medd., 1952,26(14)2 Lipas P O,Davidson J P. Nucl. Phys., 1961,26: 80 3 Davidson J P. Nucl. Phys., 1962,33:664 4 Davidson M G. Nucl. Phys., 1965,69:455 5 Philips W R,Hmad I A, Emling H et al., Phys. Rev. Lett., 1986,57: 3257 6 Urban W,Philips W R,Durell J L et al., Phys. Rev., 1997,C54:945 7 GUO JianYou et al. High Energy Phys. and Nucl. Phys. (in Chinese),2000,24(8): 780(郭建友等.高能物理与核物理,2000,24(8):780)
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GUO JianYou, RUAN TuNan and XU FuXin. Collective Motion of a pure Octupole Deformed System[J]. Chinese Physics C, 2000, 24(12): 1194-1198.
GUO JianYou, RUAN TuNan and XU FuXin. Collective Motion of a pure Octupole Deformed System[J]. Chinese Physics C, 2000, 24(12): 1194-1198. shu
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Received: 2000-04-03
Revised: 1900-01-01
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Collective Motion of a pure Octupole Deformed System

    Corresponding author: GUO JianYou,
  • Department of Modern Physics, University of Science and Technology of China, Hefei 230027, China2 Department of Physics, Anhui University, Hefei 230039, China3 CCASTWorld Laboratory, Beijing 100080, China

Abstract: The collective motion of a pure octupole deformed system is treated as the vibrations in body-fixed frame and rotation of this system about the axes of lab-system,as well as the coupling between vibrations and rotation. The quantized operator of kinetic energy is derived and the collective spectra built on some special equilibrium shape are discussed.

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