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We extend the scattering theory of the Josephson effect to include a coupling of the Josephson junction to a gapless electron reservoir in the normal state. By opening up the system with a quasiparticle escape rate 1/, the supercurrent carried at zero temperature by an Andreev level at energy ₀ is reduced by a factor (2/) (2 ₀/). We make contact with recent work on "non-Hermitian Josephson junctions", by comparing this result to different proposed generalizations of the Josephson effect to non-Hermitian Hamiltonians.
C. W. J. Beenakker (Mon,) studied this question.