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We study the fermion action needed to accurately describe the low energy physics of systems including heavy quarks in lattice QCD even when the heavy fermion mass m is on the order of, or larger than, the inverse lattice spacing: m≥1/a. We carry out an expansion through first order in |→p|a (where →p is the heavy quark momentum) and all orders in $ma$, refining the analysis of the Fermilab and Tsukuba groups. We demonstrate that the spectrum of heavy quark bound states can be determined accurately through |→p|a and (ma)ⁿ for arbitrary exponent n by using a lattice action containing only three unknown coefficients: m₀, ζ, and cP (a generalization of cSW), which are functions of $ma$. In a companion paper, we show how these three coefficients can be precisely determined using nonperturbative techniques.
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Christ et al. (2007) studied this question.
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