A Monotone operator theory

L 1) for any maximal monotone F, and are contractive (i.e. We will mainly use two well-known properties of these operators. First assume W is of this form. J. (B8) Thus, we can always solve the above equation with the v term of the form W Jv =( I + D) Jv = v. (B9) This gives us a (linear) operator splitting problem with the F and G operators given in (14). C.1 Inversion via the discrete Fourier transform However, the original form (C2) is more convenient mathematically and we use that here.