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ID Quantity Beam Target Final state Q2min,
GeV2 		Q2max,
GeV2 		Wmin,
GeV 		Wmax,
GeV 		Spokespersons
E141M1 dσ/dΩ e p π+n 1.8 1.8 1.605 1.605 K. Park, V.D. Burkert, I.G. Aznauryan
E141M2 dσ/dΩ e p π+n 1.8 1.8 1.615 1.615 K. Park, V.D. Burkert, I.G. Aznauryan
E141M3 dσ/dΩ e p π+n 1.8 1.8 1.625 1.625 K. Park, V.D. Burkert, I.G. Aznauryan
E141M4 dσ/dΩ e p π+n 1.8 1.8 1.635 1.635 K. Park, V.D. Burkert, I.G. Aznauryan
E141M5 dσ/dΩ e p π+n 1.8 1.8 1.645 1.645 K. Park, V.D. Burkert, I.G. Aznauryan
E141M6 dσ/dΩ e p π+n 1.8 1.8 1.655 1.655 K. Park, V.D. Burkert, I.G. Aznauryan
E141M7 dσ/dΩ e p π+n 1.8 1.8 1.665 1.665 K. Park, V.D. Burkert, I.G. Aznauryan
E141M8 dσ/dΩ e p π+n 1.8 1.8 1.675 1.675 K. Park, V.D. Burkert, I.G. Aznauryan
E141M9 dσ/dΩ e p π+n 1.8 1.8 1.685 1.685 K. Park, V.D. Burkert, I.G. Aznauryan
E141M10 dσ/dΩ e p π+n 1.8 1.8 1.695 1.695 K. Park, V.D. Burkert, I.G. Aznauryan
E141M11 dσ/dΩ e p π+n 1.8 1.8 1.705 1.705 K. Park, V.D. Burkert, I.G. Aznauryan
E141M12 dσ/dΩ e p π+n 1.8 1.8 1.715 1.715 K. Park, V.D. Burkert, I.G. Aznauryan
E141M13 dσ/dΩ e p π+n 1.8 1.8 1.725 1.725 K. Park, V.D. Burkert, I.G. Aznauryan
E141M14 dσ/dΩ e p π+n 1.8 1.8 1.735 1.735 K. Park, V.D. Burkert, I.G. Aznauryan
E141M15 dσ/dΩ e p π+n 1.8 1.8 1.745 1.745 K. Park, V.D. Burkert, I.G. Aznauryan
E141M16 dσ/dΩ e p π+n 1.8 1.8 1.755 1.755 K. Park, V.D. Burkert, I.G. Aznauryan
E141M17 dσ/dΩ e p π+n 1.8 1.8 1.765 1.765 K. Park, V.D. Burkert, I.G. Aznauryan
E141M18 dσ/dΩ e p π+n 1.8 1.8 1.775 1.775 K. Park, V.D. Burkert, I.G. Aznauryan
E141M19 dσ/dΩ e p π+n 1.8 1.8 1.78 1.78 K. Park, V.D. Burkert, I.G. Aznauryan
E141M20 dσ/dΩ e p π+n 1.8 1.8 1.83 1.83 K. Park, V.D. Burkert, I.G. Aznauryan
E141M21 dσ/dΩ e p π+n 1.8 1.8 1.89 1.89 K. Park, V.D. Burkert, I.G. Aznauryan
E141M22 dσ/dΩ e p π+n 1.8 1.8 1.95 1.95 K. Park, V.D. Burkert, I.G. Aznauryan
E141M23 dσ/dΩ e p π+n 1.8 1.8 2.01 2.01 K. Park, V.D. Burkert, I.G. Aznauryan
E141M24 dσ/dΩ e p π+n 2.2 2.2 1.605 1.605 K. Park, V.D. Burkert, I.G. Aznauryan
E141M25 dσ/dΩ e p π+n 2.2 2.2 1.615 1.615 K. Park, V.D. Burkert, I.G. Aznauryan
E141M26 dσ/dΩ e p π+n 2.2 2.2 1.625 1.625 K. Park, V.D. Burkert, I.G. Aznauryan
E141M27 dσ/dΩ e p π+n 2.2 2.2 1.635 1.635 K. Park, V.D. Burkert, I.G. Aznauryan
E141M28 dσ/dΩ e p π+n 2.2 2.2 1.645 1.645 K. Park, V.D. Burkert, I.G. Aznauryan
E141M29 dσ/dΩ e p π+n 2.2 2.2 1.655 1.655 K. Park, V.D. Burkert, I.G. Aznauryan
E141M30 dσ/dΩ e p π+n 2.2 2.2 1.665 1.665 K. Park, V.D. Burkert, I.G. Aznauryan
E141M31 dσ/dΩ e p π+n 2.2 2.2 1.675 1.675 K. Park, V.D. Burkert, I.G. Aznauryan
E141M32 dσ/dΩ e p π+n 2.2 2.2 1.685 1.685 K. Park, V.D. Burkert, I.G. Aznauryan
E141M33 dσ/dΩ e p π+n 2.2 2.2 1.695 1.695 K. Park, V.D. Burkert, I.G. Aznauryan
E141M34 dσ/dΩ e p π+n 2.2 2.2 1.705 1.705 K. Park, V.D. Burkert, I.G. Aznauryan
E141M35 dσ/dΩ e p π+n 2.2 2.2 1.715 1.715 K. Park, V.D. Burkert, I.G. Aznauryan
E141M36 dσ/dΩ e p π+n 2.2 2.2 1.725 1.725 K. Park, V.D. Burkert, I.G. Aznauryan
E141M37 dσ/dΩ e p π+n 2.2 2.2 1.735 1.735 K. Park, V.D. Burkert, I.G. Aznauryan
E141M38 dσ/dΩ e p π+n 2.2 2.2 1.745 1.745 K. Park, V.D. Burkert, I.G. Aznauryan
E141M39 dσ/dΩ e p π+n 2.2 2.2 1.755 1.755 K. Park, V.D. Burkert, I.G. Aznauryan
E141M40 dσ/dΩ e p π+n 2.2 2.2 1.765 1.765 K. Park, V.D. Burkert, I.G. Aznauryan
E141M41 dσ/dΩ e p π+n 2.2 2.2 1.775 1.775 K. Park, V.D. Burkert, I.G. Aznauryan
E141M42 dσ/dΩ e p π+n 2.2 2.2 1.78 1.78 K. Park, V.D. Burkert, I.G. Aznauryan
E141M43 dσ/dΩ e p π+n 2.2 2.2 1.83 1.83 K. Park, V.D. Burkert, I.G. Aznauryan
E141M44 dσ/dΩ e p π+n 2.2 2.2 1.89 1.89 K. Park, V.D. Burkert, I.G. Aznauryan
E141M45 dσ/dΩ e p π+n 2.2 2.2 1.95 1.95 K. Park, V.D. Burkert, I.G. Aznauryan
E141M46 dσ/dΩ e p π+n 2.2 2.2 2.01 2.01 K. Park, V.D. Burkert, I.G. Aznauryan
E141M47 dσ/dΩ e p π+n 2.6 2.6 1.605 1.605 K. Park, V.D. Burkert, I.G. Aznauryan
E141M48 dσ/dΩ e p π+n 2.6 2.6 1.615 1.615 K. Park, V.D. Burkert, I.G. Aznauryan
E141M49 dσ/dΩ e p π+n 2.6 2.6 1.625 1.625 K. Park, V.D. Burkert, I.G. Aznauryan
E141M50 dσ/dΩ e p π+n 2.6 2.6 1.635 1.635 K. Park, V.D. Burkert, I.G. Aznauryan
E141M51 dσ/dΩ e p π+n 2.6 2.6 1.645 1.645 K. Park, V.D. Burkert, I.G. Aznauryan
E141M52 dσ/dΩ e p π+n 2.6 2.6 1.655 1.655 K. Park, V.D. Burkert, I.G. Aznauryan
E141M53 dσ/dΩ e p π+n 2.6 2.6 1.665 1.665 K. Park, V.D. Burkert, I.G. Aznauryan
E141M54 dσ/dΩ e p π+n 2.6 2.6 1.675 1.675 K. Park, V.D. Burkert, I.G. Aznauryan
E141M55 dσ/dΩ e p π+n 2.6 2.6 1.685 1.685 K. Park, V.D. Burkert, I.G. Aznauryan
E141M56 dσ/dΩ e p π+n 2.6 2.6 1.695 1.695 K. Park, V.D. Burkert, I.G. Aznauryan
E141M57 dσ/dΩ e p π+n 2.6 2.6 1.705 1.705 K. Park, V.D. Burkert, I.G. Aznauryan
E141M58 dσ/dΩ e p π+n 2.6 2.6 1.715 1.715 K. Park, V.D. Burkert, I.G. Aznauryan
E141M59 dσ/dΩ e p π+n 2.6 2.6 1.725 1.725 K. Park, V.D. Burkert, I.G. Aznauryan
E141M60 dσ/dΩ e p π+n 2.6 2.6 1.735 1.735 K. Park, V.D. Burkert, I.G. Aznauryan
E141M61 dσ/dΩ e p π+n 2.6 2.6 1.745 1.745 K. Park, V.D. Burkert, I.G. Aznauryan
E141M62 dσ/dΩ e p π+n 2.6 2.6 1.755 1.755 K. Park, V.D. Burkert, I.G. Aznauryan
E141M63 dσ/dΩ e p π+n 2.6 2.6 1.765 1.765 K. Park, V.D. Burkert, I.G. Aznauryan
E141M64 dσ/dΩ e p π+n 2.6 2.6 1.775 1.775 K. Park, V.D. Burkert, I.G. Aznauryan
E141M65 dσ/dΩ e p π+n 2.6 2.6 1.78 1.78 K. Park, V.D. Burkert, I.G. Aznauryan
E141M66 dσ/dΩ e p π+n 2.6 2.6 1.83 1.83 K. Park, V.D. Burkert, I.G. Aznauryan
E141M67 dσ/dΩ e p π+n 2.6 2.6 1.89 1.89 K. Park, V.D. Burkert, I.G. Aznauryan
E141M68 dσ/dΩ e p π+n 2.6 2.6 1.95 1.95 K. Park, V.D. Burkert, I.G. Aznauryan
E141M69 dσ/dΩ e p π+n 2.6 2.6 2.01 2.01 K. Park, V.D. Burkert, I.G. Aznauryan
E141M70 dσ/dΩ e p π+n 3.15 3.15 1.605 1.605 K. Park, V.D. Burkert, I.G. Aznauryan
E141M71 dσ/dΩ e p π+n 3.15 3.15 1.615 1.615 K. Park, V.D. Burkert, I.G. Aznauryan
E141M72 dσ/dΩ e p π+n 3.15 3.15 1.625 1.625 K. Park, V.D. Burkert, I.G. Aznauryan
E141M73 dσ/dΩ e p π+n 3.15 3.15 1.635 1.635 K. Park, V.D. Burkert, I.G. Aznauryan
E141M74 dσ/dΩ e p π+n 3.15 3.15 1.645 1.645 K. Park, V.D. Burkert, I.G. Aznauryan
E141M75 dσ/dΩ e p π+n 3.15 3.15 1.655 1.655 K. Park, V.D. Burkert, I.G. Aznauryan
E141M76 dσ/dΩ e p π+n 3.15 3.15 1.665 1.665 K. Park, V.D. Burkert, I.G. Aznauryan
E141M77 dσ/dΩ e p π+n 3.15 3.15 1.675 1.675 K. Park, V.D. Burkert, I.G. Aznauryan
E141M78 dσ/dΩ e p π+n 3.15 3.15 1.685 1.685 K. Park, V.D. Burkert, I.G. Aznauryan
E141M79 dσ/dΩ e p π+n 3.15 3.15 1.695 1.695 K. Park, V.D. Burkert, I.G. Aznauryan
E141M80 dσ/dΩ e p π+n 3.15 3.15 1.705 1.705 K. Park, V.D. Burkert, I.G. Aznauryan
E141M81 dσ/dΩ e p π+n 3.15 3.15 1.715 1.715 K. Park, V.D. Burkert, I.G. Aznauryan
E141M82 dσ/dΩ e p π+n 3.15 3.15 1.725 1.725 K. Park, V.D. Burkert, I.G. Aznauryan
E141M83 dσ/dΩ e p π+n 3.15 3.15 1.735 1.735 K. Park, V.D. Burkert, I.G. Aznauryan
E141M84 dσ/dΩ e p π+n 3.15 3.15 1.745 1.745 K. Park, V.D. Burkert, I.G. Aznauryan
E141M85 dσ/dΩ e p π+n 3.15 3.15 1.755 1.755 K. Park, V.D. Burkert, I.G. Aznauryan
E141M86 dσ/dΩ e p π+n 3.15 3.15 1.765 1.765 K. Park, V.D. Burkert, I.G. Aznauryan
E141M87 dσ/dΩ e p π+n 3.15 3.15 1.775 1.775 K. Park, V.D. Burkert, I.G. Aznauryan
E141M88 dσ/dΩ e p π+n 3.15 3.15 1.78 1.78 K. Park, V.D. Burkert, I.G. Aznauryan
E141M89 dσ/dΩ e p π+n 3.15 3.15 1.83 1.83 K. Park, V.D. Burkert, I.G. Aznauryan
E141M90 dσ/dΩ e p π+n 3.15 3.15 1.89 1.89 K. Park, V.D. Burkert, I.G. Aznauryan
E141M91 dσ/dΩ e p π+n 3.15 3.15 1.95 1.95 K. Park, V.D. Burkert, I.G. Aznauryan
E141M92 dσ/dΩ e p π+n 3.15 3.15 2.01 2.01 K. Park, V.D. Burkert, I.G. Aznauryan
E141M93 dσ/dΩ e p π+n 4.0 4.0 1.605 1.605 K. Park, V.D. Burkert, I.G. Aznauryan
E141M94 dσ/dΩ e p π+n 4.0 4.0 1.615 1.615 K. Park, V.D. Burkert, I.G. Aznauryan
E141M95 dσ/dΩ e p π+n 4.0 4.0 1.625 1.625 K. Park, V.D. Burkert, I.G. Aznauryan
E141M96 dσ/dΩ e p π+n 4.0 4.0 1.635 1.635 K. Park, V.D. Burkert, I.G. Aznauryan
E141M97 dσ/dΩ e p π+n 4.0 4.0 1.645 1.645 K. Park, V.D. Burkert, I.G. Aznauryan
E141M98 dσ/dΩ e p π+n 4.0 4.0 1.655 1.655 K. Park, V.D. Burkert, I.G. Aznauryan
E141M99 dσ/dΩ e p π+n 4.0 4.0 1.665 1.665 K. Park, V.D. Burkert, I.G. Aznauryan
E141M100 dσ/dΩ e p π+n 4.0 4.0 1.675 1.675 K. Park, V.D. Burkert, I.G. Aznauryan
Created in SINP MSU, CLAS Collaboration