Josephson phase

From Wikipedia, the free encyclopedia

In superconductivity, the Josephson phase is the difference of the phases of the quantum mechanical wave function in two superconducting electrodes forming a Josephson junction.

For example, if the macroscopic wave functions \Psi _{1} and \Psi _{2} in superconductors 1 and 2 are given by

\Psi _{1}={\sqrt  {n_{s}}}e^{{i\theta _{1}}}
\Psi _{2}={\sqrt  {n_{s}}}e^{{i\theta _{2}}}

then the Josephson phase is \phi \ {\stackrel  {{\mathrm  {def}}}{=}}\ \theta _{2}-\theta _{1}.

This article is issued from Wikipedia. The text is available under the Creative Commons Attribution/Share Alike; additional terms may apply for the media files.