Collective Motion of a pure Octupole Deformed System

GUO JianYou; RUAN TuNan; XU FuXin

Chinese Physics C> 2000, Vol. 24> Issue(12) : 1194-1198

Collective Motion of a pure Octupole Deformed System

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

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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.

References

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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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1.
沈阳化工大学材料科学与工程学院沈阳 110142

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

Received Date: 2000-04-03
Accepted Date: 1900-01-01
Available Online: 2000-12-05

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.