Abstract

We perform a first calculation for the unpolarized parton distribution function of the Δ+Δ^+ baryon using lattice QCD simulations within the framework of Large Momentum Effective Theory. Two ensembles of Nf=2+1+1N_f=2+1+1 twisted mass fermions are utilized with a pion mass of 270 MeV and 360 MeV, respectively. The baryon, which is treated as a stable single-particle state, is boosted with momentum P3P_3 with values {0.42,0.83,1.25}\{0.42,0.83,1.25\} GeV, and we utilize momentum smearing to improve the signal. The unpolarized parton distribution function of Δ+Δ^+ is obtained using a non-perturbative renormalization and a one-loop formula for the matching, with encouraging precision. In particular, we compute the d‾(x)−u‾(x)\overline{d}(x)-\overline{u}(x) asymmetry and compare it with the same quantity in the nucleon, in a first attempt towards resolving the physical mechanism responsible for generating such asymmetry.

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