Abstract
Cross sections for semi-inclusive electroproduction of charged pions (π±) from both proton and deuteron targets were measured for 0.2<x<0.5, 2<Q2<4 GeV2, 0.3<z<1, and Pt2<0.2 GeV2. For Pt<0.1 GeV, we find the azimuthal dependence to be small, as expected theoretically. For both π+ and π−, the Pt dependence from the deuteron is found to be slightly weaker than from the proton. In the context of a simple model, this implies that the initial transverse momenta width of d quarks is larger than for u quarks and, contrary to expectations, the transverse momentum width of the favored fragmentation function is larger than the unfavored one.
Highlights
Much is known about the light-cone momentum fraction, x, and virtuality scale, Q2, dependence of the up and down quark parton distribution functions (PDFs) in the nucleon
The process of semi-inclusive deep-inelastic lepton scattering (SIDIS), lN → lhX has been shown to factorize [5], in the high energy limit, into lepton-quark scattering followed by quark hadronization
The probability of producing a pion with a transverse momentum Pt relative to the virtual photon (q) direction is described by a convolution of the quark distribution fucntions and pt-dependent fragmentation functions D+(z, pt) and D−(z, pt), where pt is the transverse momentum of the the pion relative to the quark direction, with the imposed condition Pt = zkt + pt
Summary
Cross sections for semi-inclusive electroproduction of charged pions (π±) from both proton and deuteron targets were measured for 0.2 < x < 0.5, 2 < Q2 < 4 GeV2, 0.3 < z < 1, and Pt2 < 0.2 GeV2. In the context of a simple fit, the initial transverse momenta of d quarks tends to be larger than for u quarks, while the transverse momentum width of the favored fragmentation function is slightly larger than that of the unfavored function.
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