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Extension of the de Broglie-Bohm theory to the Ginzburg-Landau equation
The de Broglie-Bohm approach permits to assign well defined trajectories to
particles that obey the Schroedinger equation. We extend this approach to
electron pairs in a superconductor. In the stationary regime this extension is
completely natural; in the general case additional postulates are required.
This approach gives enlightening views for the absence of Hall effect in the
stationary regime and for the formation of permanent currents
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