THE SU2×SU2 BASIS AND THE PHYSICAL BASES FOR THE STATE VECTORS OF d-BOSON SYSTEMS AND THE TRACELESS BOSON OPERATORS (Ⅱ)

  • For obtaining a satisfactory solution to the problem of expressing explicity the SU2×SU2—representation wave functions of the existing physical bases a new methed is introduced. The two kinds of the physical bases constructed by Chacon et al., are treated in the text. The method is compared with that of paper (Ⅰ) in the concluding section.
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  • [1] 杨泽森, 高能物理与核物理, 6(1982), No.5, 在本文中记为(I).[2] E. Chbacon, M. Moshinsky and R. T. Sharp, J. Math. Phys., 17(1976), 668.[3] E. Chacon and M. Moshinsky, J. Math. Phys., 18(1977), 870.[4] S. Szpikowski and A. Gozdz, Nucl. Phys., A340(1980), 76.[5] 孙洪洲, 高能物理与核物理, 4(1980), 478.
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YANG Ze-Sen (Tse-sen Yang). THE SU2×SU2 BASIS AND THE PHYSICAL BASES FOR THE STATE VECTORS OF d-BOSON SYSTEMS AND THE TRACELESS BOSON OPERATORS (Ⅱ)[J]. Chinese Physics C, 1983, 7(2): 245-256.
YANG Ze-Sen (Tse-sen Yang). THE SU2×SU2 BASIS AND THE PHYSICAL BASES FOR THE STATE VECTORS OF d-BOSON SYSTEMS AND THE TRACELESS BOSON OPERATORS (Ⅱ)[J]. Chinese Physics C, 1983, 7(2): 245-256. shu
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Received: 1900-01-01
Revised: 1900-01-01
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THE SU2×SU2 BASIS AND THE PHYSICAL BASES FOR THE STATE VECTORS OF d-BOSON SYSTEMS AND THE TRACELESS BOSON OPERATORS (Ⅱ)

    Corresponding author: YANG Ze-Sen (Tse-sen Yang),
  • Department of Physics, Peking University

Abstract: For obtaining a satisfactory solution to the problem of expressing explicity the SU2×SU2—representation wave functions of the existing physical bases a new methed is introduced. The two kinds of the physical bases constructed by Chacon et al., are treated in the text. The method is compared with that of paper (Ⅰ) in the concluding section.

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