Since its theoretical prediction in 1962 , the tunnelling current (with no applied voltage) that arises in a system constituted by two superconductors separated by a barrier has been the subject of many scientific studies. It was quite soon discovered that the current-phase relation I=ICsin(ϕ) (where ϕ is the phase difference between the order parameter of the two superconductors) as predicted in  does not always apply, depending both on the temperature and the barrier of the system. As a matter of fact, quite different types of current-phase relation can be found using as the separating barrier either insulators, normal metals, and superconductors, or more general constrictions of different heights and widths both in condensed matter and in ultra-cold atoms experiments.
In order to better understand the mechanism at the basis of the DC Josephson effect and to model both the current-phase relation and the critical value IC, several theoretical and numerical approaches have been developed. The early works relied mostly on the Ginzburg-Landau equations , but there were also attempts to use microscopic theories  or perturbative calculations . More recently methods have been developed based on the quasi-classical Green’s functions  and the Bogoliubov-deGennes (BdG) equations .
Despite some good agreements with the experimental data , none of these approaches could be successfully applied to the following circumstances of physical interest:
over the whole temperature range from T=0 to T=Tc;
to all possible barrier widths and heights;
along (most part of) the BCS-BEC crossover.
The main reason underlying of our study of the DC Josephson effect has been to fill this gap. To this end, we have made use of a local-phase-density approximation to the BdG equations, both in its local (LPDA)  and non-local (NLPDA)  versions. Both LPDA and NLPDA approaches, which are computationally faster and less storage demanding than the BdG equations, give us the opportunity to study the behavior of the Josephson current with reliable results along the BCS side of the BCS-BEC crossover, with no limitations on the barrier width and down to low temperatures.
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