On the Heisenberg and Schrodinger Pictures  

作　　者：Shigeji Fujita James MacNabb III Akira Suzuki 

机构地区：[1]Department of Physics,University at Buffalo,State University of New York,Buffalo,USA [2]Department of Physics,Faculty of Science,Tokyo University of Science,Tokyo,Japan

出　　处：《Journal of Modern Physics》2014年第5期171-176,共6页现代物理（英文）

摘　　要：A quantum theory for a one-electron system can be developed in either Heisenberg picture or Schrodinger picture. For a many-electron system, a theory must be developed in the Heisenberg picture, and the indistinguishability and Pauli’s exclusion principle must be incorporated. The hydrogen atom energy levels are obtained by solving the Schrodinger energy eigenvalue equation, which is the most significant result obtained in the Schrodinger picture. Both boson and fermion field equations are nonlinear in the presence of a pair interaction.A quantum theory for a one-electron system can be developed in either Heisenberg picture or Schrodinger picture. For a many-electron system, a theory must be developed in the Heisenberg picture, and the indistinguishability and Pauli’s exclusion principle must be incorporated. The hydrogen atom energy levels are obtained by solving the Schrodinger energy eigenvalue equation, which is the most significant result obtained in the Schrodinger picture. Both boson and fermion field equations are nonlinear in the presence of a pair interaction.

关 键 词：Heisenberg and Schrodingier Pictures Many-Particle Systems INDISTINGUISHABILITY Second Quantization Pauli’s Exclusion Principle 

分 类 号：O1[理学—数学]