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Consider a particle described by the wave function \Psi (r,t) Calculate the time derivative \frac{\partial p(r,t)}{\partial t} in where p(r,t) is the probability density, and shows that the continuity equation \frac{\partial p(r,t)}{\partial t}+\bigtriangledown \cdot J(r,t) = 0 is valid, where the probability current J(r,t) = \frac{1}{m}Re\left [ \Psi \ast (\frac{h}{i}\bigtriangledown \Psi ) \right ] Use the Schrodinger equation.

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