Zusammenfassung
We extend the study of lowest moments, < x > and < x(2)>, of the parton distribution function of the nucleon to include those of the sea quarks; this entails a disconnected insertion calculation in lattice QCD. This is carried out on a 16(3) x 24 quenched lattice with Wilson fermion. The quark loops are calculated with Z(2) noise vectors and unbiased subtractions, and multiple nucleon sources are ...
Zusammenfassung
We extend the study of lowest moments, < x > and < x(2)>, of the parton distribution function of the nucleon to include those of the sea quarks; this entails a disconnected insertion calculation in lattice QCD. This is carried out on a 16(3) x 24 quenched lattice with Wilson fermion. The quark loops are calculated with Z(2) noise vectors and unbiased subtractions, and multiple nucleon sources are employed to reduce the statistical errors. We obtain 5 sigma signals for < x > for the u, d, and s quarks, but < x(2)> i is consistent with zero within errors. We provide results for both the connected and disconnected insertions. The perturbatively renormalized < x > for the strange quark at mu = 2 GeV is < x >(s+(s) over bar) = 0.027 +/- 0.006 which is consistent with the experimental result. The ratio of < x > for s vs u/d in the disconnected insertion with quark loops is calculated to be 0.88 +/- 0.07. This is about twice as large as the phenomenologically fitted < x >(s+($) over bar)/< x >((u) over bar)+< x >((d) over bar) from experiments where (u) over bar and (d) over bar include both the connected and disconnected insertion parts. We discuss the source and implication of this difference. [math mode missing closing $]
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