Supersymmetric generalization of Todorov's equation

A supersymmetric generalization of the quasipotential equation in the Markov–Yukawa gauge is considered. Imposition of the supersymmetric Markov–Yukawa condition on the two-particle Bethe–Salpeter amplitude yields conditions that give the transition to a one-time wave function. For this wave function, a supersymmetric three-dimensional equation is written down. The Born term of the quasipotential is found for a selfinteracting chiral superfield, and also for interaction with a massless ehiral superfield.