Chinese Physics C > 1991, Vol. 15 > Issue(6): 496-503

EFV Method with the Constraints of Time Reversal Invariance and Axial Symmetry

ZHENG Ren-Rong^,,
ZHU Shun-Quan

Southwest China Normal University Chongqing 630715

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Abstract：
Based on the general EFV method,with the constraints of time reversal invariance and axial symmetry,simplified formulas are deduced from the HFB transformation.These results make EFV a practical method in microscopic nuclear structure physics for describing arbitrary spin and parity states in both even-even and odd-odd nuclei,including states with various correlations.

References

[1]

郑仁蓉等，, 高能物理与核物理，14(1990), 1088.[2] K. W. Schmid et al., Nucl. Phys., A431(1984), 205.[3] K. W. Schmid et al., Nucl. Phys., A431(1984), 205.[4] K. W. Schmid, and F. Gruemmer, Rep. Progr, Phys., 50(1987), 731.[5] K. W. Schmid et al., Ann. Phys., (NY) 180(1987), 1.[6] Zheng Renrong, K. W. Schmid et al., Nucl. Phys., A494(1989), 214.[7] K. W. Schmid, Zheng Renrong et al., Nucl. Phys., A499(1989), 63.[8] C. Bloch, and A. Messiah, Nucl. Phys., 39(1962), 95.

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ZHENG Ren-Rong and ZHU Shun-Quan. EFV Method with the Constraints of Time Reversal Invariance and Axial Symmetry[J]. Chinese Physics C, 1991, 15(6): 496-503.

ZHENG Ren-Rong and ZHU Shun-Quan. EFV Method with the Constraints of Time Reversal Invariance and Axial Symmetry[J]. Chinese Physics C, 1991, 15(6): 496-503. shu

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Received: 1900-01-01
Revised: 1900-01-01

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沈阳化工大学材料科学与工程学院沈阳 110142

EFV Method with the Constraints of Time Reversal Invariance and Axial Symmetry

ZHENG Ren-Rong^,
ZHU Shun-Quan

Corresponding author:ZHENG Ren-Rong,

Southwest China Normal University Chongqing 630715

Received Date:1900-01-01
Accepted Date:1900-01-01
Available Online:1991-06-05

Abstract:Based on the general EFV method,with the constraints of time reversal invariance and axial symmetry,simplified formulas are deduced from the HFB transformation.These results make EFV a practical method in microscopic nuclear structure physics for describing arbitrary spin and parity states in both even-even and odd-odd nuclei,including states with various correlations.