THE ENERGY LEVELS AND THE WAVE FUNCTION AT THE ORIGIN IN A NONRELATIVISTIC BINDING POTENTIAL

  • (1) Martin's theorem about the wave function at the origin is extended to the states with l≠0. (2) The theorems about energy levels between 2s, 2p, 3d states are extended to 3s, 3p states to the first order of perturbation.
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  • [1] H. Grosse, A. Martin, Phys. Rep., 60C(lS80), 342.[2] A. Martin, Phys. Lett., 70B(1977), 192[3] V. Gupta, R. Rajaraman, Phys. Rev., D19(1979), 697.[4] Chao Kuang-Ta, Commun. in Theor. Phys., 2(1983), 1129.[5] A. Martin, Phys. Lett., 67B(1977), 330[6] H. Grosse, Phys. Lett., 68B(1977), 343.[7] 苏汝铿、梁俊, 高能物理与核物理, 5(1981), 694.[8] H. Grosse, A. Martin, Phys. Lett., 134B(1984), 368.[9] R. P. Feynman, Phys. Rev., 56(1939), 310.
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SU Ru-Keng and ZHOU Zi-Xiang. THE ENERGY LEVELS AND THE WAVE FUNCTION AT THE ORIGIN IN A NONRELATIVISTIC BINDING POTENTIAL[J]. Chinese Physics C, 1985, 9(5): 625-628.
SU Ru-Keng and ZHOU Zi-Xiang. THE ENERGY LEVELS AND THE WAVE FUNCTION AT THE ORIGIN IN A NONRELATIVISTIC BINDING POTENTIAL[J]. Chinese Physics C, 1985, 9(5): 625-628. shu
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Received: 1900-01-01
Revised: 1900-01-01
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THE ENERGY LEVELS AND THE WAVE FUNCTION AT THE ORIGIN IN A NONRELATIVISTIC BINDING POTENTIAL

    Corresponding author: SU Ru-Keng,

Abstract: (1) Martin's theorem about the wave function at the origin is extended to the states with l≠0. (2) The theorems about energy levels between 2s, 2p, 3d states are extended to 3s, 3p states to the first order of perturbation.

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