-10.0 -5.0 0.0 5.0 10.0 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 -10.0 -5.0 0.0 5.0 10.0 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 -10.0 -5.0 0.0 5.0 10.0 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 -10.0 -5.0 0.0 5.0 10.0 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 -10.0 -5.0 0.0 5.0 10.0 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 -10.0 -5.0 0.0 5.0 10.0 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 -10.0 -5.0 0.0 5.0 10.0 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 -10.0 -5.0 0.0 5.0 10.0 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 (a) (b) (c) (d) (e) (f) (g) Amplitude of the First Fiske Step ( m A) Parallel Magnetic Field (G) (h) B$_{ }$ =1.1 G B$_{ }$ =2.1 G B$_{ }$ =3.2 G B$_{ }$ =4.3 G B$_{ }$ =5.3 G B$_{ }$ =6.4 G B$_{ }$ =7.4 G B$_{ }$ =8.0 G FIG. 6: I (1) F ( B$_{‖}$ ) curves measured after the junction was cooled in perpendicular magnetic field H$_{per}$ of various values. I − max c denoting it as I max c . Similar to [16, 17], we found the deviation of the I$_{c}$ ( B$_{‖}$ ) curve from a ”vortex-free” Fraunhofer-like curve (Fig.3, open circles) and we observed a strong suppression of I max c . For each value of B$_{⊥}$ the vortex density n$_{A}$ was calculated by using Eq.(12). The dependence of the maximum Josephson critical current I max c on the density of trapped Abrikosov vortices n$_{A}$ is shown in Fig. 7 by open squares. It is well known that 14