  A new renormalization scheme is defined for fermion bilinears in QCD at non
vanishing quark masses. This new scheme, denoted RI/mSMOM, preserves the
benefits of the nonexceptional momenta introduced in the RI/SMOM scheme, and
allows a definition of renormalized composite fields away from the chiral
limit. Some properties of the scheme are investigated by performing explicit
one-loop computation in dimensional regularization.
