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This paper presents a formulation of lattice fermions applicable to all quark masses, large and small. We incorporate interactions from previous light-fermion and heavy-fermion methods, and thus ensure a smooth connection to these limiting cases. The couplings in improved actions are obtained for arbitrary fermion mass mₐ, without expansions around small- or large-mass limits. We treat both the action and external currents. By interpreting on-shell improvement criteria through the lattice theory's Hamiltonian, one finds that cutoff artifacts factorize into the form b₍ (mₐa) pa^{s₍} where p is a momentum characteristic of the system under study, s₍ is related to the dimension of the nth interaction, and b₍ (mₐa) is a bounded function, numerically always of order 1 or less. In heavy-quark systems p is typically rather smaller than the fermion mass mₐ. Therefore, artifacts of order (mₐa) ^s do not arise, even when mₐa1. An important by-product of our analysis is an interpretation of the Wilson and Sheikholeslami-Wohlert actions applied to nonrelativistic fermions.
El-Khadra et al. (Tue,) studied this question.