CLAS Physics Database

JLab | Search | Overview | Login | Edit | Register
<< previous page Search results next page >>
Click the measurement ID (identifier) to view particular measurement data
IDFinal stateQ2min, GeV2Q2max, GeV2Wmin, GeVWmax, GeVQuantitySpokespersonsTitleYear
E216M327π+π−p33.51.81.85dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M328π+π−p33.51.81.85dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M329π+π−p33.51.81.85dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M330π+π−p33.51.81.85dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M331π+π−p33.51.81.85dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M332π+π−p33.51.81.85dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M333π+π−p33.51.81.85dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M334π+π−p33.51.851.9dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M335π+π−p33.51.851.9dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M336π+π−p33.51.851.9dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M337π+π−p33.51.851.9dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M338π+π−p33.51.851.9dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M339π+π−p33.51.851.9dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M340π+π−p33.51.851.9dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M341π+π−p33.51.851.9dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M342π+π−p33.51.851.9dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M343π+π−p33.51.91.95dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M344π+π−p33.51.91.95dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M345π+π−p33.51.91.95dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M346π+π−p33.51.91.95dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M347π+π−p33.51.91.95dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M348π+π−p33.51.91.95dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M349π+π−p33.51.91.95dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M350π+π−p33.51.91.95dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M351π+π−p33.51.91.95dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M352π+π−p33.51.952dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M353π+π−p33.51.952dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M354π+π−p33.51.952dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M355π+π−p33.51.952dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M356π+π−p33.51.952dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M357π+π−p33.51.952dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M358π+π−p33.51.952dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M359π+π−p33.51.952dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M360π+π−p33.51.952dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M361π+π−p33.522.05dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M362π+π−p33.522.05dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M363π+π−p33.522.05dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M364π+π−p33.522.05dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M365π+π−p33.522.05dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M366π+π−p33.522.05dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M367π+π−p33.522.05dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M368π+π−p33.522.05dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M369π+π−p33.522.05dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M370π+π−p33.52.052.1dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M371π+π−p33.52.052.1dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M372π+π−p33.52.052.1dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M373π+π−p33.52.052.1dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M374π+π−p33.52.052.1dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M375π+π−p33.52.052.1dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M376π+π−p33.52.052.1dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M377π+π−p33.52.052.1dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M378π+π−p33.52.052.1dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M379π+π−p3.54.21.41.45dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M380π+π−p3.54.21.41.45dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M381π+π−p3.54.21.41.45dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M382π+π−p3.54.21.41.45dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M383π+π−p3.54.21.41.45dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M384π+π−p3.54.21.41.45dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M385π+π−p3.54.21.41.45dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M386π+π−p3.54.21.41.45dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M387π+π−p3.54.21.41.45dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M388π+π−p3.54.21.451.5dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M389π+π−p3.54.21.451.5dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M390π+π−p3.54.21.451.5dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M391π+π−p3.54.21.451.5dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M392π+π−p3.54.21.451.5dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M393π+π−p3.54.21.451.5dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M394π+π−p3.54.21.451.5dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M395π+π−p3.54.21.451.5dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M396π+π−p3.54.21.451.5dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M397π+π−p3.54.21.51.55dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M398π+π−p3.54.21.51.55dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M399π+π−p3.54.21.51.55dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M400π+π−p3.54.21.51.55dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M401π+π−p3.54.21.51.55dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M402π+π−p3.54.21.51.55dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M403π+π−p3.54.21.51.55dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M404π+π−p3.54.21.51.55dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M405π+π−p3.54.21.51.55dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M406π+π−p3.54.21.551.6dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M407π+π−p3.54.21.551.6dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M408π+π−p3.54.21.551.6dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M409π+π−p3.54.21.551.6dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M410π+π−p3.54.21.551.6dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M411π+π−p3.54.21.551.6dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M412π+π−p3.54.21.551.6dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M413π+π−p3.54.21.551.6dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M414π+π−p3.54.21.551.6dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M415π+π−p3.54.21.61.65dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M416π+π−p3.54.21.61.65dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M417π+π−p3.54.21.61.65dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M418π+π−p3.54.21.61.65dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M419π+π−p3.54.21.61.65dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M420π+π−p3.54.21.61.65dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M421π+π−p3.54.21.61.65dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M422π+π−p3.54.21.61.65dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M423π+π−p3.54.21.61.65dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M424π+π−p3.54.21.651.7dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M425π+π−p3.54.21.651.7dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M426π+π−p3.54.21.651.7dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018