CLAS Physics Database

JLab | Search | Overview | Login | Edit | Register
Search results next page >>
Click the measurement ID (identifier) to view particular measurement data
IDFinal stateQ2min, GeV2Q2max, GeV2Wmin, GeVWmax, GeVQuantitySpokespersonsTitleYear
E216M127π+πp2.431.41.45dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018
E216M128π+πp2.431.41.45dσ/dM(π+)Krishna ChandraCLAS12 Run Group A2018
E216M129π+πp2.431.41.45dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M130π+πp2.431.41.45dσ/dψ(π)Krishna ChandraCLAS12 Run Group A2018
E216M131π+πp2.431.41.45dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M132π+πp2.431.41.45dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M133π+πp2.431.41.45dσ/d(−cos(θ(π)))Krishna ChandraCLAS12 Run Group A2018
E216M134π+πp2.431.41.45dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M135π+πp2.431.41.45dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M136π+πp2.431.451.5dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018
E216M137π+πp2.431.451.5dσ/dM(π+)Krishna ChandraCLAS12 Run Group A2018
E216M138π+πp2.431.451.5dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M139π+πp2.431.451.5dσ/dψ(π)Krishna ChandraCLAS12 Run Group A2018
E216M140π+πp2.431.451.5dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M141π+πp2.431.451.5dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M142π+πp2.431.451.5dσ/d(−cos(θ(π)))Krishna ChandraCLAS12 Run Group A2018
E216M143π+πp2.431.451.5dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M144π+πp2.431.451.5dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M145π+πp2.431.51.55dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018
E216M146π+πp2.431.51.55dσ/dM(π+)Krishna ChandraCLAS12 Run Group A2018
E216M147π+πp2.431.51.55dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M148π+πp2.431.51.55dσ/dψ(π)Krishna ChandraCLAS12 Run Group A2018
E216M149π+πp2.431.51.55dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M150π+πp2.431.51.55dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M151π+πp2.431.51.55dσ/d(−cos(θ(π)))Krishna ChandraCLAS12 Run Group A2018
E216M152π+πp2.431.51.55dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M153π+πp2.431.51.55dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M154π+πp2.431.551.6dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018
E216M155π+πp2.431.551.6dσ/dM(π+)Krishna ChandraCLAS12 Run Group A2018
E216M156π+πp2.431.551.6dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M157π+πp2.431.551.6dσ/dψ(π)Krishna ChandraCLAS12 Run Group A2018
E216M158π+πp2.431.551.6dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M159π+πp2.431.551.6dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M160π+πp2.431.551.6dσ/d(−cos(θ(π)))Krishna ChandraCLAS12 Run Group A2018
E216M161π+πp2.431.551.6dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M162π+πp2.431.551.6dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M163π+πp2.431.61.65dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018
E216M164π+πp2.431.61.65dσ/dM(π+)Krishna ChandraCLAS12 Run Group A2018
E216M165π+πp2.431.61.65dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M166π+πp2.431.61.65dσ/dψ(π)Krishna ChandraCLAS12 Run Group A2018
E216M167π+πp2.431.61.65dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M168π+πp2.431.61.65dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M169π+πp2.431.61.65dσ/d(−cos(θ(π)))Krishna ChandraCLAS12 Run Group A2018
E216M170π+πp2.431.61.65dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M171π+πp2.431.61.65dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M172π+πp2.431.651.7dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018
E216M173π+πp2.431.651.7dσ/dM(π+)Krishna ChandraCLAS12 Run Group A2018
E216M174π+πp2.431.651.7dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M175π+πp2.431.651.7dσ/dψ(π)Krishna ChandraCLAS12 Run Group A2018
E216M176π+πp2.431.651.7dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M177π+πp2.431.651.7dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M178π+πp2.431.651.7dσ/d(−cos(θ(π)))Krishna ChandraCLAS12 Run Group A2018
E216M179π+πp2.431.651.7dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M180π+πp2.431.651.7dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M181π+πp2.431.71.75dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018
E216M182π+πp2.431.71.75dσ/dM(π+)Krishna ChandraCLAS12 Run Group A2018
E216M183π+πp2.431.71.75dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M184π+πp2.431.71.75dσ/dψ(π)Krishna ChandraCLAS12 Run Group A2018
E216M185π+πp2.431.71.75dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M186π+πp2.431.71.75dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M187π+πp2.431.71.75dσ/d(−cos(θ(π)))Krishna ChandraCLAS12 Run Group A2018
E216M188π+πp2.431.71.75dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M189π+πp2.431.71.75dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M190π+πp2.431.751.8dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018
E216M191π+πp2.431.751.8dσ/dM(π+)Krishna ChandraCLAS12 Run Group A2018
E216M192π+πp2.431.751.8dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M193π+πp2.431.751.8dσ/dψ(π)Krishna ChandraCLAS12 Run Group A2018
E216M194π+πp2.431.751.8dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M195π+πp2.431.751.8dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M196π+πp2.431.751.8dσ/d(−cos(θ(π)))Krishna ChandraCLAS12 Run Group A2018
E216M197π+πp2.431.751.8dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M198π+πp2.431.751.8dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M199π+πp2.431.81.85dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018
E216M200π+πp2.431.81.85dσ/dM(π+)Krishna ChandraCLAS12 Run Group A2018
E216M201π+πp2.431.81.85dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M202π+πp2.431.81.85dσ/dψ(π)Krishna ChandraCLAS12 Run Group A2018
E216M203π+πp2.431.81.85dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M204π+πp2.431.81.85dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M205π+πp2.431.81.85dσ/d(−cos(θ(π)))Krishna ChandraCLAS12 Run Group A2018
E216M206π+πp2.431.81.85dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M207π+πp2.431.81.85dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M208π+πp2.431.851.9dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018
E216M209π+πp2.431.851.9dσ/dM(π+)Krishna ChandraCLAS12 Run Group A2018
E216M210π+πp2.431.851.9dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M211π+πp2.431.851.9dσ/dψ(π)Krishna ChandraCLAS12 Run Group A2018
E216M212π+πp2.431.851.9dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M213π+πp2.431.851.9dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M214π+πp2.431.851.9dσ/d(−cos(θ(π)))Krishna ChandraCLAS12 Run Group A2018
E216M215π+πp2.431.851.9dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M216π+πp2.431.851.9dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M217π+πp2.431.91.95dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018
E216M218π+πp2.431.91.95dσ/dM(π+)Krishna ChandraCLAS12 Run Group A2018
E216M219π+πp2.431.91.95dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M220π+πp2.431.91.95dσ/dψ(π)Krishna ChandraCLAS12 Run Group A2018
E216M221π+πp2.431.91.95dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M222π+πp2.431.91.95dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M223π+πp2.431.91.95dσ/d(−cos(θ(π)))Krishna ChandraCLAS12 Run Group A2018
E216M224π+πp2.431.91.95dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M225π+πp2.431.91.95dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M226π+πp2.431.952dσ/dM(π,p)Krishna ChandraCLAS12 Run Group A2018