-10.0 -5.0 0.0 5.0 10.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.5 -10.0 -5.0 0.0 5.0 10.0 -1.2 -0.9 -0.6 -0.3 0.0 0.3 0.6 0.9 1.2 -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 -0.8 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 0.8 -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 -0.4 -0.3 -0.2 -0.1 0.0 0.1 0.2 0.3 0.4 -10.0 -5.0 0.0 5.0 10.0 -0.4 -0.3 -0.2 -0.1 0.0 0.1 0.2 0.3 0.4 (a) (b) (c) (d) (e) (f) (g) Josephson Critical Current (m A) Parallel M agnetic 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. 5: I$_{c}$ ( B$_{‖}$ ) curves measured after cooling of the junction in perpendicular magnetic field B$_{⊥}$ of various values. C. Josephson critical current of a junction with trapped Abrikosov vortices Fig.5 shows I$_{c}$ ( B$_{‖}$ ) curves measured after cooling of the sample in different perpendicular magnetic fields B$_{⊥}$ . We obtained from each I$_{c}$ ( B$_{‖}$ ) curve the maximum values of I$_{c}$ for both polarities, I + max c and I − max c , and then we selected the maximum value between I + max c and 13