CLAS Physics Database

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IDFinal stateQ2min, GeV2Q2max, GeV2Wmin, GeVWmax, GeVQuantitySpokespersonsTitleYear
E216M627π+π−p4.252.052.1dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M628π+π−p4.252.052.1dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M629π+π−p4.252.052.1dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M630π+π−p4.252.052.1dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M631π+π−p561.41.45dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M632π+π−p561.41.45dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M633π+π−p561.41.45dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M634π+π−p561.41.45dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M635π+π−p561.41.45dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M636π+π−p561.41.45dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M637π+π−p561.41.45dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M638π+π−p561.41.45dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M639π+π−p561.41.45dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M640π+π−p561.451.5dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M641π+π−p561.451.5dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M642π+π−p561.451.5dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M643π+π−p561.451.5dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M644π+π−p561.451.5dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M645π+π−p561.451.5dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M646π+π−p561.451.5dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M647π+π−p561.451.5dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M648π+π−p561.451.5dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M649π+π−p561.51.55dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M650π+π−p561.51.55dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M651π+π−p561.51.55dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M652π+π−p561.51.55dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M653π+π−p561.51.55dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M654π+π−p561.51.55dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M655π+π−p561.51.55dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M656π+π−p561.51.55dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M657π+π−p561.51.55dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M658π+π−p561.551.6dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M659π+π−p561.551.6dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M660π+π−p561.551.6dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M661π+π−p561.551.6dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M662π+π−p561.551.6dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M663π+π−p561.551.6dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M664π+π−p561.551.6dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M665π+π−p561.551.6dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M666π+π−p561.551.6dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M667π+π−p561.61.65dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M668π+π−p561.61.65dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M669π+π−p561.61.65dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M670π+π−p561.61.65dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M671π+π−p561.61.65dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M672π+π−p561.61.65dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M673π+π−p561.61.65dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M674π+π−p561.61.65dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M675π+π−p561.61.65dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M676π+π−p561.651.7dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M677π+π−p561.651.7dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M678π+π−p561.651.7dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M679π+π−p561.651.7dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M680π+π−p561.651.7dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M681π+π−p561.651.7dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M682π+π−p561.651.7dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M683π+π−p561.651.7dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M684π+π−p561.651.7dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M685π+π−p561.71.75dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M686π+π−p561.71.75dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M687π+π−p561.71.75dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M688π+π−p561.71.75dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M689π+π−p561.71.75dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M690π+π−p561.71.75dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M691π+π−p561.71.75dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M692π+π−p561.71.75dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M693π+π−p561.71.75dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M694π+π−p561.751.8dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M695π+π−p561.751.8dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M696π+π−p561.751.8dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M697π+π−p561.751.8dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M698π+π−p561.751.8dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M699π+π−p561.751.8dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M700π+π−p561.751.8dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M701π+π−p561.751.8dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M702π+π−p561.751.8dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M703π+π−p561.81.85dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M704π+π−p561.81.85dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M705π+π−p561.81.85dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M706π+π−p561.81.85dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M707π+π−p561.81.85dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M708π+π−p561.81.85dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M709π+π−p561.81.85dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M710π+π−p561.81.85dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M711π+π−p561.81.85dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M712π+π−p561.851.9dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M713π+π−p561.851.9dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M714π+π−p561.851.9dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M715π+π−p561.851.9dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M716π+π−p561.851.9dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M717π+π−p561.851.9dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M718π+π−p561.851.9dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M719π+π−p561.851.9dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M720π+π−p561.851.9dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M721π+π−p561.91.95dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M722π+π−p561.91.95dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M723π+π−p561.91.95dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M724π+π−p561.91.95dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M725π+π−p561.91.95dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M726π+π−p561.91.95dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018