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  MNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard

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  这时（3）全同粒子的交换不变性的后果 A．两全同粒子的波函数 若两全同粒子它们的相互作用是变量可 分离型的即 N为奇 因此在一级近似下

• QD22.ppt

  MNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard

• QD05.ppt

  MNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard

• QD15.ppt

  MNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard

• QD27.ppt

  MNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard

• QD24.ppt

  MNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard

• QD23.ppt

  MNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard

• QD28.ppt

  MNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard

• QD29.ppt

  MNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard Route –_QD_DetailsMNSOFT Standard