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ID Quantity Beam Target Final state Q2min,
GeV2 		Q2max,
GeV2 		Wmin,
GeV 		Wmax,
GeV 		Spokespersons
E187M75 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.1125 1.1125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M76 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.1125 1.1125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M77 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.1375 1.1375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M78 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.1375 1.1375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M79 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.1375 1.1375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M80 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.1625 1.1625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M81 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.1625 1.1625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M82 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.1625 1.1625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M83 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.1875 1.1875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M84 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.1875 1.1875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M85 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.1875 1.1875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M86 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.2125 1.2125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M87 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.2125 1.2125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M88 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.2125 1.2125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M89 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.2375 1.2375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M90 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.2375 1.2375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M91 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.2375 1.2375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M92 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.2625 1.2625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M93 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.2625 1.2625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M94 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.2625 1.2625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M95 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.2875 1.2875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M96 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.2875 1.2875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M97 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.2875 1.2875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M98 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.3125 1.3125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M99 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.3125 1.3125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M100 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.3125 1.3125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M101 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.3375 1.3375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M102 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.3375 1.3375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M103 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.3375 1.3375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M104 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.3625 1.3625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M105 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.3625 1.3625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M106 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.3625 1.3625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M107 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.3875 1.3875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M108 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.3875 1.3875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M109 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.3875 1.3875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M110 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.4125 1.4125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M111 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.4125 1.4125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M112 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.4125 1.4125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M113 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.4375 1.4375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M114 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.4375 1.4375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M115 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.4375 1.4375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M116 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.4625 1.4625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M117 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.4625 1.4625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M118 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.4625 1.4625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M119 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.4875 1.4875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M120 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.4875 1.4875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M121 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.4875 1.4875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M122 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.5125 1.5125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M123 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.5125 1.5125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M124 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.5125 1.5125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M125 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.5375 1.5375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M126 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.5375 1.5375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M127 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.5375 1.5375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M128 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.5625 1.5625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M129 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.5625 1.5625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M130 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.5625 1.5625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M131 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.5875 1.5875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M132 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.5875 1.5875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M133 dσ/dΩ (quasi-free) e d π− p 0.9 0.9 1.5875 1.5875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M134 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.6125 1.6125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M135 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.6125 1.6125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M136 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.6375 1.6375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M137 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.6375 1.6375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M138 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.6625 1.6625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M139 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.6625 1.6625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M140 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.6875 1.6875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M141 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.6875 1.6875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M142 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.7125 1.7125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M143 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.7125 1.7125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M144 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.7375 1.7375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M145 dσ/dΩ (quasi-free) e d π− p 0.7 0.7 1.7375 1.7375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M146 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.7625 1.7625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M147 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.7875 1.7875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M148 dσ/dΩ (quasi-free) e d π− p 0.5 0.5 1.8125 1.8125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
Created in SINP MSU, CLAS Collaboration