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Published in:
1999 | OriginalPaper | Chapter
General Concepts
Author : Prof. Dr. Siegfried Flügge
Published in: Practical Quantum Mechanics
Publisher: Springer Berlin Heidelberg
Included in: Professional Book Archive
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If the normalization relation (1.1)$$\int {{d^3}} x\psi * \psi = 1$$is interpreted in the sense of probability theory, so that $${d^3}x\psi * \psi$$ is the probability of finding the particle under consideration in the volume element d3x, then there must be a conservation law. This is to be derived. How may it be interpreted classically?