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    • https://phys.libretexts.org/Bookshelves/Quantum_Mechanics/Essential_Graduate_Physics_-_Quantum_Mechanics_(Likharev)/09%3A_Elements_of_Relativistic_Quantum_Mechanics/9.05%3A_The_Klien-Gordon_and_Relativistic_Schrodinger_Equations
      Of more formal properties of Eq. (84), it is easy to prove that its solutions satisfy the same continuity equation (1.52), with the probability current density j still given by Eq. (1.47)...Of more formal properties of Eq. (84), it is easy to prove that its solutions satisfy the same continuity equation (1.52), with the probability current density j still given by Eq. (1.47), but a different expression for the probability density w - which becomes very similar to that for j : \[w=\frac{i \hbar}{2 m c^{2}}\left(\Psi^{*} \frac{\partial \Psi}{\partial t}-\text { c.c. }\right), \quad \mathbf{j}=\frac{i \hbar}{2 m}\left(\Psi \nabla \Psi^{*}-\text { c.c. }\…

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