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IDFinal stateQ2min, GeV2Q2max, GeV2Wmin, GeVWmax, GeVQuantitySpokespersonsTitleYear
E216M527π+π−p4.251.51.55dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M528π+π−p4.251.51.55dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M529π+π−p4.251.51.55dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M530π+π−p4.251.51.55dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M531π+π−p4.251.51.55dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M532π+π−p4.251.551.6dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M533π+π−p4.251.551.6dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M534π+π−p4.251.551.6dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M535π+π−p4.251.551.6dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M536π+π−p4.251.551.6dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M537π+π−p4.251.551.6dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M538π+π−p4.251.551.6dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M539π+π−p4.251.551.6dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M540π+π−p4.251.551.6dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M541π+π−p4.251.61.65dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M542π+π−p4.251.61.65dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M543π+π−p4.251.61.65dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M544π+π−p4.251.61.65dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M545π+π−p4.251.61.65dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M546π+π−p4.251.61.65dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M547π+π−p4.251.61.65dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M548π+π−p4.251.61.65dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M549π+π−p4.251.61.65dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M550π+π−p4.251.651.7dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M551π+π−p4.251.651.7dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M552π+π−p4.251.651.7dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M553π+π−p4.251.651.7dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M554π+π−p4.251.651.7dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M555π+π−p4.251.651.7dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M556π+π−p4.251.651.7dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M557π+π−p4.251.651.7dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M558π+π−p4.251.651.7dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M559π+π−p4.251.71.75dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M560π+π−p4.251.71.75dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M561π+π−p4.251.71.75dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M562π+π−p4.251.71.75dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M563π+π−p4.251.71.75dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M564π+π−p4.251.71.75dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M565π+π−p4.251.71.75dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M566π+π−p4.251.71.75dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M567π+π−p4.251.71.75dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M568π+π−p4.251.751.8dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M569π+π−p4.251.751.8dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M570π+π−p4.251.751.8dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M571π+π−p4.251.751.8dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M572π+π−p4.251.751.8dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M573π+π−p4.251.751.8dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M574π+π−p4.251.751.8dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M575π+π−p4.251.751.8dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M576π+π−p4.251.751.8dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M577π+π−p4.251.81.85dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M578π+π−p4.251.81.85dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M579π+π−p4.251.81.85dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M580π+π−p4.251.81.85dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M581π+π−p4.251.81.85dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M582π+π−p4.251.81.85dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M583π+π−p4.251.81.85dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M584π+π−p4.251.81.85dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M585π+π−p4.251.81.85dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M586π+π−p4.251.851.9dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M587π+π−p4.251.851.9dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M588π+π−p4.251.851.9dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M589π+π−p4.251.851.9dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M590π+π−p4.251.851.9dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M591π+π−p4.251.851.9dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M592π+π−p4.251.851.9dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M593π+π−p4.251.851.9dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M594π+π−p4.251.851.9dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M595π+π−p4.251.91.95dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M596π+π−p4.251.91.95dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M597π+π−p4.251.91.95dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M598π+π−p4.251.91.95dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M599π+π−p4.251.91.95dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M600π+π−p4.251.91.95dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M601π+π−p4.251.91.95dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M602π+π−p4.251.91.95dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M603π+π−p4.251.91.95dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M604π+π−p4.251.952dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M605π+π−p4.251.952dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M606π+π−p4.251.952dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M607π+π−p4.251.952dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M608π+π−p4.251.952dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M609π+π−p4.251.952dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M610π+π−p4.251.952dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M611π+π−p4.251.952dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M612π+π−p4.251.952dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M613π+π−p4.2522.05dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M614π+π−p4.2522.05dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M615π+π−p4.2522.05dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M616π+π−p4.2522.05dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M617π+π−p4.2522.05dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M618π+π−p4.2522.05dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M619π+π−p4.2522.05dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M620π+π−p4.2522.05dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M621π+π−p4.2522.05dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M622π+π−p4.252.052.1dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M623π+π−p4.252.052.1dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M624π+π−p4.252.052.1dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M625π+π−p4.252.052.1dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M626π+π−p4.252.052.1dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018