Fig.1 Dependence of the differential cross section of d(e,e'p)n reaction on the angle of the momentum
         of spectator neutron with respect to the q.  Black curves within virtual nucleon approximation,
         with de Forest 1 and red curves within light cone approximation. Dashed lines are PWIA and solid
         lines are PWIA+ FSI calculations. Red dotted line shows the limit, below(left) of which the incoming
         momentum of final state pn system < 500 MeV/c. Green dotted line shows the limit, below of which
         the incoming momentum of final state pn system < 1000 MeV/c

Fig.2 Dependence of the differential cross section of d(e,e'p)n reaction on the angle of the momentum
         of spectator neutron with respect to the q.  Black curves within virtual nucleon approximation,
         with de Forest 1 and red curves within light cone approximation. Dashed lines are PWIA and
         solid lines are PWIA+ FSI calculations. Green dotted line shows the limit, below of which the
         incoming  momentum of final state pn system < 1000 MeV/c
 
 
 
 
 

Fig.3 Dependence of the differential cross section of d(e,e'p)n reaction on the angle of the momentum
         of spectator neutron with respect to the q.  Black curves within virtual nucleon approximation,
         with de Forest 1 and red curves within light cone approximation. Dashed lines are PWIA and solid
         lines are PWIA+ FSI calculations. Red dotted line shows the limit, below of which the incoming
         momentum of final state pn system < 500 MeV/c Green dotted line shows the limit, below of which
         the incoming momentum of final state pn system < 1000 MeV/c