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The systematics of kinematic moment of inertia J~((1))and dynamic moment of inertia J~((2))of superdeformed(SD) bands in A~130, 150, 190 mass regions have been studied. We have obtained the values of J~((1))and J~((2))for all the SD bands observed in the A~130, 150, 190 mass regions by using the experimental intraband E2 transition energies. The result of this work includes the variation of J~((1))with the product of valence proton and neutron numbers(N_pN_n). The phenomenon of band mixing has been observed in the A~130, 150 mass regions and band crossing has been observed in the A~190 mass region. The systematics also includes the variation of J~((2))with the product of valence proton and neutron numbers(N_pN_n). Evidence of staggering behaviour has been observed in all three A~130, 150 and 190 mass regions. We present for the first time the variation of J~((1))and J~((2))of SD bands in the A~130, 150, 190 mass regions with N_pN_n.
The systematics of kinematic moment of inertia J ~ ((1)) and dynamic moment of inertia J ~ ((2)) of superdeformed (SD) bands in A ~ 130, 150, 190 mass regions have been studied. values of J ~ ((1)) and J ~ ((2)) for all the SD bands were observed in the A ~ 130, 150, 190 mass regions by using the experimental intraband E2 transition energies. The result of this work includes the variation of J ~ ((1)) with the product of valence proton and neutron numbers (N_pN_n). The phenomenon of band mixing has been observed in the A ~ 130, 150 mass regions and band crossing has been observed in the A ~ 190 mass region. The systematics also includes the variation of J ~ ((2)) with the product of valence proton and neutron numbers (N_pN_n). Evidence of staggering behavior has been observed in all three A ~ 130, 150 and 190 mass regions. We present for the first time the variation of J ~ ((1)) and J ~ ((2)) of SD bands in the A ~ 130, 150, 190 mass regions with N_pN_n.