Massive Fermions in Lattice Gauge Theory

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 evaluated for arbitrary fermion mass~$m_q$, 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 $b_n(m_{q}a)[\text{vek}pa{]}^{s_n}$, where $\text{vek}p$ is a momentum characteristic of the system under study, $s_n$ is related to the dimension of the $n$th interaction, and $b_n(m_{q}a)$ is a bounded function, numerically always~$\text{order}(1)$ or less. In heavy-quark systems $\text{vek}p$ is typically rather smaller than the fermion mass~$m_q$. Therefore, artifacts of order $(m_{q}a{)}^s$ do not arise, even when $m_{q}a\text{gsim}1$. An important by-product of our analysis is an interpretation of the Wilson and Sheikholeslami-Wohlert actions applied to nonrelativistic fermions.