A superconducting weak link is a connection between regions with superconductivity whose coupling is weak enough that a substantial difference of quantum phase can develop across the connection. An insulating tunnel barrier is one realization; a narrow conducting constriction can also couple the regions. The current-phase relation of a superconducting weak link depends on the connection. A sinusoid is the leading tunnel-junction approximation, not a universal law for every superconducting weak link. [ref]
The Discovery of Tunnelling Supercurrents by Brian D. Josephson. Josephson, Nobel lecture (12 December 1973), final discussion of weak links and tunnel barriers
The current-phase relation of a superconducting weak link gives its pair electric current as a function of the Gauge-invariant Josephson phase , at specified temperature and other conditions. For the ideal junction used below, with . More general periodic relations can contain higher Fourier harmonics; their maximum magnitude defines the corresponding superconducting critical current.
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