CLAS Physics Database

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Click the measurement ID (identifier) to view particular measurement data
IDFinal stateQ2min, GeV2Q2max, GeV2Wmin, GeVWmax, GeVQuantitySpokespersonsTitleYear
E216M427π+π−p3.54.21.651.7dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M428π+π−p3.54.21.651.7dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M429π+π−p3.54.21.651.7dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M430π+π−p3.54.21.651.7dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M431π+π−p3.54.21.651.7dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M432π+π−p3.54.21.651.7dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M433π+π−p3.54.21.71.75dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M434π+π−p3.54.21.71.75dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M435π+π−p3.54.21.71.75dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M436π+π−p3.54.21.71.75dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M437π+π−p3.54.21.71.75dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M438π+π−p3.54.21.71.75dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M439π+π−p3.54.21.71.75dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M440π+π−p3.54.21.71.75dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M441π+π−p3.54.21.71.75dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M442π+π−p3.54.21.751.8dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M443π+π−p3.54.21.751.8dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M444π+π−p3.54.21.751.8dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M445π+π−p3.54.21.751.8dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M446π+π−p3.54.21.751.8dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M447π+π−p3.54.21.751.8dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M448π+π−p3.54.21.751.8dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M449π+π−p3.54.21.751.8dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M450π+π−p3.54.21.751.8dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M451π+π−p3.54.21.81.85dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M452π+π−p3.54.21.81.85dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M453π+π−p3.54.21.81.85dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M454π+π−p3.54.21.81.85dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M455π+π−p3.54.21.81.85dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M456π+π−p3.54.21.81.85dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M457π+π−p3.54.21.81.85dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M458π+π−p3.54.21.81.85dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M459π+π−p3.54.21.81.85dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M460π+π−p3.54.21.851.9dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M461π+π−p3.54.21.851.9dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M462π+π−p3.54.21.851.9dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M463π+π−p3.54.21.851.9dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M464π+π−p3.54.21.851.9dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M465π+π−p3.54.21.851.9dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M466π+π−p3.54.21.851.9dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M467π+π−p3.54.21.851.9dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M468π+π−p3.54.21.851.9dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M469π+π−p3.54.21.91.95dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M470π+π−p3.54.21.91.95dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M471π+π−p3.54.21.91.95dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M472π+π−p3.54.21.91.95dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M473π+π−p3.54.21.91.95dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M474π+π−p3.54.21.91.95dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M475π+π−p3.54.21.91.95dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M476π+π−p3.54.21.91.95dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M477π+π−p3.54.21.91.95dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M478π+π−p3.54.21.952dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M479π+π−p3.54.21.952dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M480π+π−p3.54.21.952dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M481π+π−p3.54.21.952dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M482π+π−p3.54.21.952dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M483π+π−p3.54.21.952dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M484π+π−p3.54.21.952dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M485π+π−p3.54.21.952dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M486π+π−p3.54.21.952dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M487π+π−p3.54.222.05dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M488π+π−p3.54.222.05dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M489π+π−p3.54.222.05dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M490π+π−p3.54.222.05dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M491π+π−p3.54.222.05dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M492π+π−p3.54.222.05dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M493π+π−p3.54.222.05dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M494π+π−p3.54.222.05dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M495π+π−p3.54.222.05dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M496π+π−p3.54.22.052.1dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M497π+π−p3.54.22.052.1dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M498π+π−p3.54.22.052.1dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M499π+π−p3.54.22.052.1dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M500π+π−p3.54.22.052.1dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M501π+π−p3.54.22.052.1dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M502π+π−p3.54.22.052.1dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M503π+π−p3.54.22.052.1dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M504π+π−p3.54.22.052.1dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M505π+π−p4.251.41.45dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M506π+π−p4.251.41.45dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M507π+π−p4.251.41.45dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M508π+π−p4.251.41.45dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M509π+π−p4.251.41.45dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M510π+π−p4.251.41.45dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M511π+π−p4.251.41.45dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M512π+π−p4.251.41.45dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M513π+π−p4.251.41.45dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M514π+π−p4.251.451.5dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M515π+π−p4.251.451.5dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M516π+π−p4.251.451.5dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M517π+π−p4.251.451.5dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018
E216M518π+π−p4.251.451.5dσ/dψ(π+)Krishna ChandraCLAS12 Run Group A2018
E216M519π+π−p4.251.451.5dσ/dψ(p)Krishna ChandraCLAS12 Run Group A2018
E216M520π+π−p4.251.451.5dσ/d(−cos(θ(π−)))Krishna ChandraCLAS12 Run Group A2018
E216M521π+π−p4.251.451.5dσ/d(−cos(θ(π+)))Krishna ChandraCLAS12 Run Group A2018
E216M522π+π−p4.251.451.5dσ/d(−cos(θ(p)))Krishna ChandraCLAS12 Run Group A2018
E216M523π+π−p4.251.51.55dσ/dM(π−,p)Krishna ChandraCLAS12 Run Group A2018
E216M524π+π−p4.251.51.55dσ/dM(π+,π−)Krishna ChandraCLAS12 Run Group A2018
E216M525π+π−p4.251.51.55dσ/dM(π+,p)Krishna ChandraCLAS12 Run Group A2018
E216M526π+π−p4.251.51.55dσ/dψ(π−)Krishna ChandraCLAS12 Run Group A2018