CLAS Physics Database

Search results

ID Quantity Beam Target Final state Q2min,
GeV2
Q2max,
GeV2
Wmin,
GeV
Wmax,
GeV
Spokespersons
E187M1 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.1125 1.1125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M2 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.1125 1.1125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M3 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.1375 1.1375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M4 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.1375 1.1375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M5 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.1375 1.1375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M6 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.1625 1.1625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M7 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.1625 1.1625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M8 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.1625 1.1625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M9 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.1875 1.1875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M10 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.1875 1.1875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M11 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.1875 1.1875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M12 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.2125 1.2125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M13 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.2125 1.2125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M14 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.2125 1.2125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M15 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.2375 1.2375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M16 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.2375 1.2375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M17 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.2375 1.2375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M18 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.2625 1.2625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M19 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.2625 1.2625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M20 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.2625 1.2625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M21 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.2875 1.2875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M22 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.2875 1.2875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M23 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.2875 1.2875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M24 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.3125 1.3125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M25 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.3125 1.3125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M26 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.3125 1.3125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M27 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.3375 1.3375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M28 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.3375 1.3375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M29 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.3375 1.3375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M30 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.3625 1.3625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M31 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.3625 1.3625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M32 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.3625 1.3625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M33 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.3875 1.3875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M34 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.3875 1.3875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M35 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.3875 1.3875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M36 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.4125 1.4125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M37 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.4125 1.4125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M38 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.4125 1.4125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M39 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.4375 1.4375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M40 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.4375 1.4375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M41 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.4375 1.4375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M42 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.4625 1.4625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M43 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.4625 1.4625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M44 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.4625 1.4625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M45 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.4875 1.4875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M46 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.4875 1.4875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M47 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.4875 1.4875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M48 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.5125 1.5125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M49 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.5125 1.5125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M50 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.5125 1.5125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M51 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.5375 1.5375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M52 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.5375 1.5375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M53 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.5375 1.5375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M54 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.5625 1.5625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M55 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.5625 1.5625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M56 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.5625 1.5625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M57 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.5875 1.5875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M58 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.5875 1.5875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M59 dσ/dΩ (exclusive) e d π p 0.9 0.9 1.5875 1.5875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M60 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.6125 1.6125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M61 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.6125 1.6125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M62 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.6375 1.6375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M63 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.6375 1.6375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M64 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.6625 1.6625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M65 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.6625 1.6625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M66 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.6875 1.6875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M67 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.6875 1.6875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M68 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.7125 1.7125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M69 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.7125 1.7125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M70 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.7375 1.7375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M71 dσ/dΩ (exclusive) e d π p 0.7 0.7 1.7375 1.7375 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M72 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.7625 1.7625 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M73 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.7875 1.7875 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis
E187M74 dσ/dΩ (exclusive) e d π p 0.5 0.5 1.8125 1.8125 Y. Tian, R. W. Gothe V.I. Mokeev, and G. Hollis