Gauge Dependence of Effective Quark Mass and Matrix Elements in Gaugefixed Large N Strong Coupling Lattice QCD

In conjunction with recent numerical \hbox{$\lambda~\partial_0 A_0 + \nabla\cdot\vec{A} =0$} ``$\lambda$-gauge'' results reported in a companion paper, we construct an $N\to\infty$ Wilson loop picture of $\lambda$-gaugefixing in which (I)the $\lambda$-gauge expectation value of a link chain $C$ is the weighted sum over Wilson loops made by joining to $C$ all selfavoiding chains $\widetilde{C}$ closing $C$. (II)Weights $A_{\widetilde{C}}$, containing all the $\lambda$-dependence, are given by the $\beta=0$ $\lambda$-gauge expectation value of $\widetilde{C}$. (III)$A_{\widetilde{C}}$ equals path-products of coefficients from the trace expansion of the gaugefixing Boltzmann weight. From (II) and (III) we deduce formulas for $\beta =0$ quark matrix elements. We find that $M_q^{(\lambda)}$ decreases with increasing $\lambda$; the quark propagator dispersion relation is not covariant when $\lambda\ne 1$; and $\Delta I=1/2$ matching coefficients are $\lambda$-independent. These strong coupling features are qualitatively consistent with numerical $\beta=5.7$ and $6.0$ results briefly described here for comparison purposes but mainly presented in a companion paper.