content_image/337609.jpg
<img src='content_image/337609.jpg'>

for the junction in the absence of Abrikosov vortices, was not convenient for the case of trapped Abrikosov vortices. We used γ as a fitting parameter in order to reach the good agreement between the experimental value of I (1) F recorded at B$_{⊥}$ = 1 . 1 G and the theoretical value calculated by using Eq. (4) and Eq. (5) for the same magnetic field. We obtain γ = 2 . 2 × 10 10 s − 1 from this fitting procedure and the parameter σ ∗ = 3 . 2 × 10 2 µm 2 was estimated. It is important to note that the quality factor Q = ω$_{0}$/γ of the Fiske resonance is equal to 31, such that a crucial assumption of low dissipative junctions is valid for our junctions. 

Using Eq. (7) we calculated the correlation area σ for each value of density n$_{A}$ , and we 

