The study of boundary value problems involving linear differentiai equations with real-valued coefficients is by now a well-established area of analysis. On the other hand, much less is known about the solvability of such problems when the coefficients (or boundary conditions) are known to be complex. Examples of this latter type arise naturally, for example, in nuclear physics (e.g., the so-called optical mode1 for low energy scattering [ 1, p. IjO]), electromagnetic field theory (dielectric waveguides with heat loss (c.f. 19 I), or the propagation of radio waves through inhomogeneous media [S]), and elsewhere. In cases like these, the relevant differential expressions are no longer formally symmetric, and hence the powerful methods associated with the spectral theory of selfadjoint operators are not available. To facilitate the study of such problems, Glazman introduced in [4] the concept of a J-symmetric operator: In a complex Hilbert space R, let J be a given conjugation operator on 2’ (i.e., J is a conjugate-linear involution with (Jx, 3~) = (u, x) for all x and y in 2). A closed, densely defined linear operator T in 3’ is said to be J-symmetric if