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Photoproduction Of The F(1)(1285) Meson
Photoproduction Of The F(1)(1285) Meson
Measurements Of The Gamma(upsilon)p -> P 'pi(+)pi(- )cross Section With The Clas Detector For 0.4 Gev2 < Q(2) < 1.0 Gev2 And 1.3 Gev < W < 1.825 Gev
Measurements Of The Gamma(upsilon)p -> P 'pi(+)pi(- )cross Section With The Clas Detector For 0.4 Gev2 < Q(2) < 1.0 Gev2 And 1.3 Gev < W < 1.825 Gev
Measurement Of Emission-angle Anisotropy Via Long-range Angular Correlations With High-pt Hadrons In D Plus Au And P Plus P Collisions At Root S(nn)=200 Gev
Measurement Of Emission-angle Anisotropy Via Long-range Angular Correlations With High-pt Hadrons In D Plus Au And P Plus P Collisions At Root S(nn)=200 Gev
First Measurement Of Xi(-) Polarization In Photoproduction
First Measurement Of Xi(-) Polarization In Photoproduction
Center Of Mass Motion Of Short-range Correlated Nucleon Pairs Studied Via The A(e,e ' Pp) Reaction
Center Of Mass Motion Of Short-range Correlated Nucleon Pairs Studied Via The A(e,e ' Pp) Reaction
Exclusive Photoproduction Of Pi Degrees Up To Large Values Of Mandelstam Variables S, T, And U With Clas
Exclusive Photoproduction Of Pi Degrees Up To Large Values Of Mandelstam Variables S, T, And U With Clas
Exclusive Eta Electroproduction At W > 2 Gev With Clas And Transversity Generalized Parton Distributions
Exclusive Eta Electroproduction At W > 2 Gev With Clas And Transversity Generalized Parton Distributions
Semi-inclusive Pi(0) Target And Beam-target Asymmetries From 6 Gev Electron Scattering With Clas
Semi-inclusive Pi(0) Target And Beam-target Asymmetries From 6 Gev Electron Scattering With Clas
Measurement Of Target And Double-spin Asymmetries For The (e)over-right-arrow (p)over-right-arrow -> E Pi(+)(n) Reaction In The Nucleon Resonance Region At Low Q(2)
Measurement Of Target And Double-spin Asymmetries For The (e)over-right-arrow (p)over-right-arrow -> E Pi(+)(n) Reaction In The Nucleon Resonance Region At Low Q(2)
Target And Double Spin Asymmetries Of Deeply Virtual Pi(0) Production With A Longitudinally Polarized Proton Target And Clas
Target And Double Spin Asymmetries Of Deeply Virtual Pi(0) Production With A Longitudinally Polarized Proton Target And Clas
Differential Cross Section For Gamma D -> Omega D Using Clas At Jefferson Lab
Differential Cross Section For Gamma D -> Omega D Using Clas At Jefferson Lab
Exclusive Pi(0)p Electroproduction Off Protons In The Resonance Region At Photon Virtualities 0.4 Gev2 <= Q(2) <= 1 Gev2
Exclusive Pi(0)p Electroproduction Off Protons In The Resonance Region At Photon Virtualities 0.4 Gev2 <= Q(2) <= 1 Gev2
First measurement of the helicity asymmetry E in eta photoproduction on the proton
First measurement of the helicity asymmetry E in eta photoproduction on the proton
Centrality-Dependent Modification of Jet-Production Rates in Deuteron-Gold Collisions at root s(NN)=200 GeV
Centrality-Dependent Modification of Jet-Production Rates in Deuteron-Gold Collisions at root s(NN)=200 GeV
Target And Beam-target Spin Asymmetries In Exclusive Pion Electroproduction For Q(2) > 1 Gev2. I. Ep -> E Pi(+)n
Target And Beam-target Spin Asymmetries In Exclusive Pion Electroproduction For Q(2) > 1 Gev2. I. Ep -> E Pi(+)n
Measurement Of The Beam Asymmetry Sigma And The Target Asymmetry T In The Photoproduction Of Omega Mesons Off The Proton Using Clas At Jefferson Laboratory
Measurement Of The Beam Asymmetry Sigma And The Target Asymmetry T In The Photoproduction Of Omega Mesons Off The Proton Using Clas At Jefferson Laboratory
Transverse Energy Production And Charged-particle Multiplicity At Midrapidity In Various Systems From Root S(nn)=7.7 To 200 Gev
Transverse Energy Production And Charged-particle Multiplicity At Midrapidity In Various Systems From Root S(nn)=7.7 To 200 Gev
Photoproduction Of K+ K- Meson Pairs On The Proton
Photoproduction Of K+ K- Meson Pairs On The Proton
Target And Beam-target Spin Asymmetries In Exclusive Pion Electroproduction For Q(2) > 1 Gev2. Ii. Ep -> E Pi(0) P
Target And Beam-target Spin Asymmetries In Exclusive Pion Electroproduction For Q(2) > 1 Gev2. Ii. Ep -> E Pi(0) P