| Modern physics |
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| [math]\displaystyle{ \hat{H} | \psi_n(t) \rangle = i \hbar \frac{\partial}{\partial t} | \psi_n(t) \rangle }[/math] [math]\displaystyle{ \frac { 1 }{ { c }^{ 2 } } \frac { { \partial }^{ 2 }{ \phi }_{n} }{ { \partial t }^{ 2 } } -{ { \nabla }^{ 2 }{ \phi }_{n} }+{ \left( \frac { mc }{ \hbar } \right) }^{ 2 }{ \phi }_{n}=0 }[/math] |
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