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
E216M827π+π−p671.751.8dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M828π+π−p671.751.8dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M829π+π−p671.81.85dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M830π+π−p671.81.85dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M831π+π−p671.81.85dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M832π+π−p671.81.85dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M833π+π−p671.81.85dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M834π+π−p671.81.85dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M835π+π−p671.81.85dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M836π+π−p671.81.85dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M837π+π−p671.81.85dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M838π+π−p671.851.9dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M839π+π−p671.851.9dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M840π+π−p671.851.9dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M841π+π−p671.851.9dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M842π+π−p671.851.9dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M843π+π−p671.851.9dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M844π+π−p671.851.9dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M845π+π−p671.851.9dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M846π+π−p671.851.9dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M847π+π−p671.91.95dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M848π+π−p671.91.95dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M849π+π−p671.91.95dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M850π+π−p671.91.95dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M851π+π−p671.91.95dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M852π+π−p671.91.95dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M853π+π−p671.91.95dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M854π+π−p671.91.95dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M855π+π−p671.91.95dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M856π+π−p671.952dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M857π+π−p671.952dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M858π+π−p671.952dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M859π+π−p671.952dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M860π+π−p671.952dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M861π+π−p671.952dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M862π+π−p671.952dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M863π+π−p671.952dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M864π+π−p671.952dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M865π+π−p6722.05dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M866π+π−p6722.05dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M867π+π−p6722.05dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M868π+π−p6722.05dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M869π+π−p6722.05dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M870π+π−p6722.05dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M871π+π−p6722.05dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M872π+π−p6722.05dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M873π+π−p6722.05dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M874π+π−p672.052.1dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M875π+π−p672.052.1dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M876π+π−p672.052.1dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M877π+π−p672.052.1dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M878π+π−p672.052.1dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M879π+π−p672.052.1dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M880π+π−p672.052.1dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M881π+π−p672.052.1dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M882π+π−p672.052.1dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M883π+π−p781.41.45dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M884π+π−p781.41.45dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M885π+π−p781.41.45dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M886π+π−p781.41.45dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M887π+π−p781.41.45dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M888π+π−p781.41.45dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M889π+π−p781.41.45dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M890π+π−p781.41.45dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M891π+π−p781.41.45dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M892π+π−p781.451.5dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M893π+π−p781.451.5dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M894π+π−p781.451.5dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M895π+π−p781.451.5dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M896π+π−p781.451.5dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M897π+π−p781.451.5dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M898π+π−p781.451.5dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M899π+π−p781.451.5dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M900π+π−p781.451.5dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M901π+π−p781.51.55dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M902π+π−p781.51.55dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M903π+π−p781.51.55dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M904π+π−p781.51.55dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M905π+π−p781.51.55dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M906π+π−p781.51.55dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M907π+π−p781.51.55dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M908π+π−p781.51.55dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M909π+π−p781.51.55dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M910π+π−p781.551.6dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M911π+π−p781.551.6dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M912π+π−p781.551.6dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M913π+π−p781.551.6dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M914π+π−p781.551.6dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M915π+π−p781.551.6dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M916π+π−p781.551.6dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M917π+π−p781.551.6dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M918π+π−p781.551.6dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M919π+π−p781.61.65dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M920π+π−p781.61.65dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M921π+π−p781.61.65dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M922π+π−p781.61.65dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M923π+π−p781.61.65dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M924π+π−p781.61.65dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M925π+π−p781.61.65dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M926π+π−p781.61.65dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018