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\left(\beta路mc^{2}+c\left(\sum路_{n{\mathop路
{=}}1}^{3}\alpha路_{n}p_{n}\right)\right)\psi路(x,t)=i\hbar路
{\frac路{\partial路\psi路(x,t)}{\partial路t}}露
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\left(\beta mc^{2}+c\left(\sum _{n{\mathop {=}}1}^{3}\alpha _{n}p_{n}\right)\right)\psi (x,t)=i\hbar {\frac {\partial \psi (x,t)}{\partial t}}
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Author: Anonymous User 1167