Abstract

We study diquarks on the lattice in the background of a static quark, in a gauge-invariant formalism with quark masses down to almost physical mπm_π. We determine mass differences between diquark channels as well as diquark-quark mass differences. The lightest and next-to-lightest diquarks have "good" scalar, 3ˉF\bar{3}_F, 3ˉc\bar{3}_c, JP=0+J^P=0^+, and "bad" axial vector, 6F6_F, 3ˉc\bar{3}_c, JP=1+J^P=1^+, quantum numbers, and a bad-good mass difference for udud flavors, 198(4) MeV198(4)~\rm{MeV}, in excellent agreement with phenomenological determinations. Quark-quark attraction is found only in the "good" diquark channel. We extract a corresponding diquark size of ∼0.6 fm\sim 0.6~\rm{fm} and perform a first exploration of the "good" diquark shape, which is shown to be spherical. Our results provide quantitative support for modeling the low-lying baryon spectrum using good light diquark effective degrees of freedom.

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