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IDFinal stateQ2min, GeV2Q2max, GeV2Wmin, GeVWmax, GeVQuantitySpokespersonsTitleYear
E216M127π+π−p2.431.41.45dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M128π+π−p2.431.41.45dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M129π+π−p2.431.41.45dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M130π+π−p2.431.41.45dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M131π+π−p2.431.41.45dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M132π+π−p2.431.41.45dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M133π+π−p2.431.41.45dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M134π+π−p2.431.41.45dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M135π+π−p2.431.41.45dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M136π+π−p2.431.451.5dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M137π+π−p2.431.451.5dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M138π+π−p2.431.451.5dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M139π+π−p2.431.451.5dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M140π+π−p2.431.451.5dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M141π+π−p2.431.451.5dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M142π+π−p2.431.451.5dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M143π+π−p2.431.451.5dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M144π+π−p2.431.451.5dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M145π+π−p2.431.51.55dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M146π+π−p2.431.51.55dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M147π+π−p2.431.51.55dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M148π+π−p2.431.51.55dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M149π+π−p2.431.51.55dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M150π+π−p2.431.51.55dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M151π+π−p2.431.51.55dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M152π+π−p2.431.51.55dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M153π+π−p2.431.51.55dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M154π+π−p2.431.551.6dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M155π+π−p2.431.551.6dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M156π+π−p2.431.551.6dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M157π+π−p2.431.551.6dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M158π+π−p2.431.551.6dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M159π+π−p2.431.551.6dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M160π+π−p2.431.551.6dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M161π+π−p2.431.551.6dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M162π+π−p2.431.551.6dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M163π+π−p2.431.61.65dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M164π+π−p2.431.61.65dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M165π+π−p2.431.61.65dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M166π+π−p2.431.61.65dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M167π+π−p2.431.61.65dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M168π+π−p2.431.61.65dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M169π+π−p2.431.61.65dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M170π+π−p2.431.61.65dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M171π+π−p2.431.61.65dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M172π+π−p2.431.651.7dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M173π+π−p2.431.651.7dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M174π+π−p2.431.651.7dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M175π+π−p2.431.651.7dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M176π+π−p2.431.651.7dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M177π+π−p2.431.651.7dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M178π+π−p2.431.651.7dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M179π+π−p2.431.651.7dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M180π+π−p2.431.651.7dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M181π+π−p2.431.71.75dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M182π+π−p2.431.71.75dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M183π+π−p2.431.71.75dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M184π+π−p2.431.71.75dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M185π+π−p2.431.71.75dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M186π+π−p2.431.71.75dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M187π+π−p2.431.71.75dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M188π+π−p2.431.71.75dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M189π+π−p2.431.71.75dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M190π+π−p2.431.751.8dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M191π+π−p2.431.751.8dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M192π+π−p2.431.751.8dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M193π+π−p2.431.751.8dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M194π+π−p2.431.751.8dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M195π+π−p2.431.751.8dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M196π+π−p2.431.751.8dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M197π+π−p2.431.751.8dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M198π+π−p2.431.751.8dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M199π+π−p2.431.81.85dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M200π+π−p2.431.81.85dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M201π+π−p2.431.81.85dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M202π+π−p2.431.81.85dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M203π+π−p2.431.81.85dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M204π+π−p2.431.81.85dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M205π+π−p2.431.81.85dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M206π+π−p2.431.81.85dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M207π+π−p2.431.81.85dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M208π+π−p2.431.851.9dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M209π+π−p2.431.851.9dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M210π+π−p2.431.851.9dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M211π+π−p2.431.851.9dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M212π+π−p2.431.851.9dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M213π+π−p2.431.851.9dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M214π+π−p2.431.851.9dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M215π+π−p2.431.851.9dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M216π+π−p2.431.851.9dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M217π+π−p2.431.91.95dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M218π+π−p2.431.91.95dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M219π+π−p2.431.91.95dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M220π+π−p2.431.91.95dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M221π+π−p2.431.91.95dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M222π+π−p2.431.91.95dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M223π+π−p2.431.91.95dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M224π+π−p2.431.91.95dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M225π+π−p2.431.91.95dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M226π+π−p2.431.952dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018