Summary
The theory of the relativistic Schrödinger equations is further elaborated: the integrability conditions for the existence of a wave function ψ(x) directly lead to the general situation where a wave function («pure state») is not available to describe the physical system.
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References
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Mattes, M., Sorg, M. Integrability conditions, wave functions, and conservation laws for the relativistic Schrödinger equations. Nuov Cim B 109, 1097–1111 (1994). https://doi.org/10.1007/BF02723233
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DOI: https://doi.org/10.1007/BF02723233