-
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
[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)
|
-
[1] |
PENG Quan-Ling
, SUN Jian
, ZHAO Guang-Yuan
, SHI Cai-Tu
. Principle and Software Design of Helmhotz Coil Measurement System. Chinese Physics C,
2001, 25(9): 920-925. |
[2] |
Xu Jianming
. Matching Problem of Lattice with Transverse Coupling. Chinese Physics C,
1995, 19(1): 73-81. |
[3] |
HOU Ren-Chang
, ZHAO Xuan
. QUADRUPOLE-OCTUPOLE TWO-PHONON EXCITATIONS IN INELASTIC SCATTERING. Chinese Physics C,
1983, 7(2): 236-244. |
-
Access
-
-