CLAS Physics Database

CLAS12 RG-K

Spokesperson
Daniel S. Carman
Year
2022
Abstract
Beam-recoil transferred polarization integrated over all Phi angles.
Publication
  1. D. S. Carman et al. (CLAS Collaboration) Beam-recoil transferred polarization in K + Y electroproduction in the nucleon resonance region with CLAS12 // https://journals.aps.org/prc/abstract/10.1103/PhysRevC.105.065201
Quantities
P′x P′z P′x′ P′z′

Measurements

ID Quantity Beam Target Final state Q2min,
GeV2
Q2max,
GeV2
Wmin,
GeV
Wmax,
GeV
E195M101 P′z′ e p K+ Λ 1.0 4.5 1.6 2.4
E195M102 P′z′ e p K+ Λ 1.0 4.5 1.6 2.4
E195M103 P′z′ e p K+ Λ 1.0 4.5 1.6 2.4
E195M104 P′z′ e p K+ Λ 1.0 4.5 1.6 2.4
E195M105 P′z e p K+ Λ 0.4 1.0 1.6 2.4
E195M106 P′z e p K+ Λ 0.4 1.0 1.6 2.4
E195M107 P′z e p K+ Λ 0.4 1.0 1.6 2.4
E195M108 P′z e p K+ Λ 0.4 1.0 1.6 2.4
E195M109 P′z e p K+ Λ 1.0 4.5 1.6 2.4
E195M110 P′z e p K+ Λ 1.0 4.5 1.6 2.4
E195M111 P′z e p K+ Λ 1.0 4.5 1.6 2.4
E195M112 P′z e p K+ Λ 1.0 4.5 1.6 2.4
E195M113 P′x′ e p K+ Σ0 0.3 0.9 1.6 2.4
E195M114 P′x′ e p K+ Σ0 0.3 0.9 1.6 2.4
E195M115 P′x′ e p K+ Σ0 0.3 0.9 1.6 2.4
E195M116 P′x′ e p K+ Σ0 0.3 0.9 1.6 2.4
E195M117 P′x′ e p K+ Σ0 0.9 3.5 1.6 2.4
E195M118 P′x′ e p K+ Σ0 0.9 3.5 1.6 2.4
E195M119 P′x′ e p K+ Σ0 0.9 3.5 1.6 2.4
E195M120 P′x′ e p K+ Σ0 0.9 3.5 1.6 2.4
E195M121 P′x e p K+ Σ0 0.3 0.9 1.6 2.4
E195M122 P′x e p K+ Σ0 0.3 0.9 1.6 2.4
E195M123 P′x e p K+ Σ0 0.3 0.9 1.6 2.4
E195M124 P′x e p K+ Σ0 0.3 0.9 1.6 2.4
E195M125 P′x e p K+ Σ0 0.9 3.5 1.6 2.4
E195M126 P′x e p K+ Σ0 0.9 3.5 1.6 2.4
E195M127 P′x e p K+ Σ0 0.9 3.5 1.6 2.4
E195M128 P′x e p K+ Σ0 0.9 3.5 1.6 2.4
E195M129 P′z′ e p K+ Σ0 0.3 0.9 1.6 2.4
E195M130 P′z′ e p K+ Σ0 0.3 0.9 1.6 2.4
E195M131 P′z′ e p K+ Σ0 0.3 0.9 1.6 2.4
E195M132 P′z′ e p K+ Σ0 0.3 0.9 1.6 2.4
E195M133 P′z′ e p K+ Σ0 0.9 3.5 1.6 2.4
E195M134 P′z′ e p K+ Σ0 0.9 3.5 1.6 2.4
E195M135 P′z′ e p K+ Σ0 0.9 3.5 1.6 2.4
E195M136 P′z′ e p K+ Σ0 0.9 3.5 1.6 2.4
E195M137 P′z e p K+ Σ0 0.3 0.9 1.6 2.4
E195M138 P′z e p K+ Σ0 0.3 0.9 1.6 2.4
E195M139 P′z e p K+ Σ0 0.3 0.9 1.6 2.4
E195M140 P′z e p K+ Σ0 0.3 0.9 1.6 2.4
E195M141 P′z e p K+ Σ0 0.9 3.5 1.6 2.4
E195M142 P′z e p K+ Σ0 0.9 3.5 1.6 2.4
E195M143 P′z e p K+ Σ0 0.9 3.5 1.6 2.4
E195M144 P′z e p K+ Σ0 0.9 3.5 1.6 2.4
E195M145 P′x′ e p K+ Σ0 0.4 1.0 1.6 2.4
E195M146 P′x′ e p K+ Σ0 0.4 1.0 1.6 2.4
E195M147 P′x′ e p K+ Σ0 0.4 1.0 1.6 2.4
E195M148 P′x′ e p K+ Σ0 0.4 1.0 1.6 2.4
E195M149 P′x′ e p K+ Σ0 1.0 4.5 1.6 2.4
E195M150 P′x′ e p K+ Σ0 1.0 4.5 1.6 2.4
E195M151 P′x′ e p K+ Σ0 1.0 4.5 1.6 2.4
E195M152 P′x′ e p K+ Σ0 1.0 4.5 1.6 2.4
E195M153 P′x e p K+ Σ0 0.4 1.0 1.6 2.4
E195M154 P′x e p K+ Σ0 0.4 1.0 1.6 2.4
E195M155 P′x e p K+ Σ0 0.4 1.0 1.6 2.4
E195M156 P′x e p K+ Σ0 0.4 1.0 1.6 2.4
E195M157 P′x e p K+ Σ0 1.0 4.5 1.6 2.4
E195M158 P′x e p K+ Σ0 1.0 4.5 1.6 2.4
E195M159 P′x e p K+ Σ0 1.0 4.5 1.6 2.4
E195M160 P′x e p K+ Σ0 1.0 4.5 1.6 2.4
E195M161 P′z′ e p K+ Σ0 0.4 1.0 1.6 2.4
E195M162 P′z′ e p K+ Σ0 0.4 1.0 1.6 2.4
E195M163 P′z′ e p K+ Σ0 0.4 1.0 1.6 2.4
E195M164 P′z′ e p K+ Σ0 0.4 1.0 1.6 2.4
E195M165 P′z′ e p K+ Σ0 1.0 4.5 1.6 2.4
E195M166 P′z′ e p K+ Σ0 1.0 4.5 1.6 2.4
E195M167 P′z′ e p K+ Σ0 1.0 4.5 1.6 2.4
E195M168 P′z′ e p K+ Σ0 1.0 4.5 1.6 2.4
E195M169 P′z e p K+ Σ0 0.4 1.0 1.6 2.4
E195M170 P′z e p K+ Σ0 0.4 1.0 1.6 2.4
E195M171 P′z e p K+ Σ0 0.4 1.0 1.6 2.4
E195M172 P′z e p K+ Σ0 0.4 1.0 1.6 2.4
E195M173 P′z e p K+ Σ0 1.0 4.5 1.6 2.4
E195M174 P′z e p K+ Σ0 1.0 4.5 1.6 2.4
E195M175 P′z e p K+ Σ0 1.0 4.5 1.6 2.4
E195M176 P′z e p K+ Σ0 1.0 4.5 1.6 2.4