User:Hillgentleman/Postulates of quantum mechanics

量子力學嘅公設：

量子態可由波函數代表 ([LL],p.6)

重疊原則 ([LL], p.7)

兩個無相干嘅系統嘅波函數，係兩支獨立波函數嘅積 ([LL], p.7)

量度([LL,p.3])一量子態$\sum a_{i}f_{i}$，出嘅結果係eigenstate $f_{0}$嘅機會係 $a_{0}^{2}$。

參攷

• Landau/Lifschitz (1998), Quantum Mechanics (non relativistic theory) (Course of Theoretical Physics, Vol.3) , ISBN 0080291406

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