CLAS Physics Database

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Click the measurement ID (identifier) to view particular measurement data
IDFinal stateQ2min, GeV2Q2max, GeV2Wmin, GeVWmax, GeVQuantitySpokespersonsTitleYear
E216M727π+π−p561.91.95dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M728π+π−p561.91.95dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M729π+π−p561.91.95dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M730π+π−p561.952dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M731π+π−p561.952dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M732π+π−p561.952dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M733π+π−p561.952dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M734π+π−p561.952dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M735π+π−p561.952dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M736π+π−p561.952dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M737π+π−p561.952dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M738π+π−p561.952dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M739π+π−p5622.05dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M740π+π−p5622.05dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M741π+π−p5622.05dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M742π+π−p5622.05dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M743π+π−p5622.05dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M744π+π−p5622.05dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M745π+π−p5622.05dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M746π+π−p5622.05dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M747π+π−p5622.05dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M748π+π−p562.052.1dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M749π+π−p562.052.1dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M750π+π−p562.052.1dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M751π+π−p562.052.1dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M752π+π−p562.052.1dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M753π+π−p562.052.1dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M754π+π−p562.052.1dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M755π+π−p562.052.1dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M756π+π−p562.052.1dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M757π+π−p671.41.45dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M758π+π−p671.41.45dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M759π+π−p671.41.45dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M760π+π−p671.41.45dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M761π+π−p671.41.45dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M762π+π−p671.41.45dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M763π+π−p671.41.45dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M764π+π−p671.41.45dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M765π+π−p671.41.45dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M766π+π−p671.451.5dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M767π+π−p671.451.5dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M768π+π−p671.451.5dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M769π+π−p671.451.5dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M770π+π−p671.451.5dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M771π+π−p671.451.5dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M772π+π−p671.451.5dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M773π+π−p671.451.5dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M774π+π−p671.451.5dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M775π+π−p671.51.55dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M776π+π−p671.51.55dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M777π+π−p671.51.55dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M778π+π−p671.51.55dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M779π+π−p671.51.55dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M780π+π−p671.51.55dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M781π+π−p671.51.55dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M782π+π−p671.51.55dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M783π+π−p671.51.55dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M784π+π−p671.551.6dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M785π+π−p671.551.6dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M786π+π−p671.551.6dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M787π+π−p671.551.6dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M788π+π−p671.551.6dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M789π+π−p671.551.6dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M790π+π−p671.551.6dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M791π+π−p671.551.6dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M792π+π−p671.551.6dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M793π+π−p671.61.65dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M794π+π−p671.61.65dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M795π+π−p671.61.65dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M796π+π−p671.61.65dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M797π+π−p671.61.65dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M798π+π−p671.61.65dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M799π+π−p671.61.65dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M800π+π−p671.61.65dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M801π+π−p671.61.65dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M802π+π−p671.651.7dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M803π+π−p671.651.7dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M804π+π−p671.651.7dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M805π+π−p671.651.7dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M806π+π−p671.651.7dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M807π+π−p671.651.7dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M808π+π−p671.651.7dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M809π+π−p671.651.7dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M810π+π−p671.651.7dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M811π+π−p671.71.75dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M812π+π−p671.71.75dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M813π+π−p671.71.75dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M814π+π−p671.71.75dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M815π+π−p671.71.75dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M816π+π−p671.71.75dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M817π+π−p671.71.75dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M818π+π−p671.71.75dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M819π+π−p671.71.75dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M820π+π−p671.751.8dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M821π+π−p671.751.8dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M822π+π−p671.751.8dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M823π+π−p671.751.8dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M824π+π−p671.751.8dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M825π+π−p671.751.8dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M826π+π−p671.751.8dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018