0.0 0.1 0.2 0.3 0.4 0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6  - Max. Josephson Critical C u rrent (mA)  - Max. Amplitude of the First Fi s ke Step (mA) Abrikosov Vortex Density ( m$^{-2}$) FIG. 7: Open squares: Experimental dependence of the maximum Josephson critical current I max c on the density of trapped Abrikosov vortices n ; Open circles: Experimental dependence of the maximum amplitude of the first Fiske step I (1) ,max F on the density of trapped Abrikosov vortices n . Solid line is the theoretical I (1) ,max F ( n$_{A}$ ) curve, calculated by Eqs.(11) and (7). The values of γ = 2 . 2 × 10 s − 1 and a mean misalignment parameter over all vortex densities δ = 0 . 8 µm were used; Full circles represent the theoretical I F 1 ,max c ( n$_{A}$ ) dependence obtained by Eqs.(11) and (8). 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 16