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Long Josephson junction : ウィキペディア英語版
Long Josephson junction

In superconductivity, a long Josephson junction (LJJ) is a Josephson junction which has one or more dimensions longer than the Josephson penetration depth \lambda_J. This definition is not strict.
In terms of underlying model a ''short Josephson junction'' is characterized by the Josephson phase \phi(t), which is only a function of time, but not of coordinates i.e. the Josephson junction is assumed to be point-like in space. In contrast, in a long Josephson junction the Josephson phase can be a function of one or two spatial coordinates, i.e., \phi(x,t) or \phi(x,y,t).
==Simple model: the sine-Gordon equation==
The simplest and the most frequently used model which describes the dynamics of the Josephson phase \phi in LJJ is the so-called perturbed sine-Gordon equation. For the case of 1D LJJ it looks like:

\lambda_J^2\phi_-\omega_p^\phi_-\sin(\phi)
=\omega_c^\phi_t - j/j_c,

where subscripts x and t denote partial derivatives with respect to x and t, \lambda_J is the Josephson penetration depth, \omega_p is the Josephson plasma frequency, \omega_c is the so-called characteristic frequency and j/j_c is the bias current density j normalized to the critical current density j_c. In the above equation, the r.h.s. is considered as perturbation.
Usually for theoretical studies one uses normalized sine-Gordon equation:

\phi_-\phi_-\sin(\phi)=\alpha\phi_t - \gamma,

where spatial coordinate is normalized to the Josephson penetration depth \lambda_J and time is normalized to the inverse plasma frequency \omega_p^. The parameter \alpha=1/\sqrt is the dimensionless damping parameter (\beta_c is McCumber-Stewart parameter), and, finally, \gamma=j/j_c is a normalized bias current.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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