Abstract
In the staggered fermion formulation of lattice QCD, we construct and classify the diquark operators to be embedded in the singly heavy baryons, $qqQ$. Along the same manner as in the staggered meson classifications given in [M. F. L. Golterman, Nucl. Phys. B273, 663 (1986).], we establish the group theoretical connections between continuum and lattice staggered diquark representations.
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