CLAS Physics Database

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Search results

ID Quantity Beam Target Final state Q2min,
GeV2 		Q2max,
GeV2 		Wmin,
GeV 		Wmax,
GeV 		Spokespersons
E1M1 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.4 1.425 V. D. Burkert, M. Ripani
E1M14 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.425 1.45 V. D. Burkert, M. Ripani
E1M27 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.45 1.475 V. D. Burkert, M. Ripani
E1M38 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.475 1.5 V. D. Burkert, M. Ripani
E1M51 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.5 1.525 V. D. Burkert, M. Ripani
E1M70 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.525 1.55 V. D. Burkert, M. Ripani
E1M74 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.55 1.575 V. D. Burkert, M. Ripani
E1M86 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.575 1.6 V. D. Burkert, M. Ripani
E1M100 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.6 1.625 V. D. Burkert, M. Ripani
E1M111 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.625 1.65 V. D. Burkert, M. Ripani
E1M122 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.65 1.675 V. D. Burkert, M. Ripani
E1M134 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.675 1.7 V. D. Burkert, M. Ripani
E1M148 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.7 1.725 V. D. Burkert, M. Ripani
E1M160 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.725 1.75 V. D. Burkert, M. Ripani
E1M172 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.75 1.775 V. D. Burkert, M. Ripani
E1M184 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.775 1.8 V. D. Burkert, M. Ripani
E1M198 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.8 1.825 V. D. Burkert, M. Ripani
E1M210 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.825 1.85 V. D. Burkert, M. Ripani
E1M216 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.85 1.875 V. D. Burkert, M. Ripani
E1M234 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.875 1.9 V. D. Burkert, M. Ripani
E1M240 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.9 1.925 V. D. Burkert, M. Ripani
E1M252 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.925 1.95 V. D. Burkert, M. Ripani
E1M264 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.95 1.975 V. D. Burkert, M. Ripani
E1M276 dσ/dM(π+,p) e p π+π−p 1.1 1.5 1.975 2.0 V. D. Burkert, M. Ripani
E1M295 dσ/dM(π+,p) e p π+π−p 1.1 1.5 2.0 2.025 V. D. Burkert, M. Ripani
E1M300 dσ/dM(π+,p) e p π+π−p 1.1 1.5 2.025 2.05 V. D. Burkert, M. Ripani
E1M314 dσ/dM(π+,p) e p π+π−p 1.1 1.5 2.05 2.075 V. D. Burkert, M. Ripani
E1M325 dσ/dM(π+,p) e p π+π−p 1.1 1.5 2.075 2.1 V. D. Burkert, M. Ripani
E1M337 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.4 1.425 V. D. Burkert, M. Ripani
E1M353 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.425 1.45 V. D. Burkert, M. Ripani
E1M364 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.45 1.475 V. D. Burkert, M. Ripani
E1M374 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.475 1.5 V. D. Burkert, M. Ripani
E1M387 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.5 1.525 V. D. Burkert, M. Ripani
E1M399 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.525 1.55 V. D. Burkert, M. Ripani
E1M411 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.55 1.575 V. D. Burkert, M. Ripani
E1M423 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.575 1.6 V. D. Burkert, M. Ripani
E1M435 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.6 1.625 V. D. Burkert, M. Ripani
E1M447 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.625 1.65 V. D. Burkert, M. Ripani
E1M459 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.65 1.675 V. D. Burkert, M. Ripani
E1M476 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.675 1.7 V. D. Burkert, M. Ripani
E1M482 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.7 1.725 V. D. Burkert, M. Ripani
E1M494 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.725 1.75 V. D. Burkert, M. Ripani
E1M506 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.75 1.775 V. D. Burkert, M. Ripani
E1M518 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.775 1.8 V. D. Burkert, M. Ripani
E1M538 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.8 1.825 V. D. Burkert, M. Ripani
E1M550 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.825 1.85 V. D. Burkert, M. Ripani
E1M562 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.85 1.875 V. D. Burkert, M. Ripani
E1M574 dσ/dM(π+,p) e p π+π−p 0.5 0.8 1.875 1.9 V. D. Burkert, M. Ripani
E1M578 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.4 1.425 V. D. Burkert, M. Ripani
E1M590 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.425 1.45 V. D. Burkert, M. Ripani
E1M602 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.45 1.475 V. D. Burkert, M. Ripani
E1M614 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.475 1.5 V. D. Burkert, M. Ripani
E1M626 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.5 1.525 V. D. Burkert, M. Ripani
E1M638 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.525 1.55 V. D. Burkert, M. Ripani
E1M650 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.55 1.575 V. D. Burkert, M. Ripani
E1M662 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.575 1.6 V. D. Burkert, M. Ripani
E1M676 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.6 1.625 V. D. Burkert, M. Ripani
E1M687 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.625 1.65 V. D. Burkert, M. Ripani
E1M700 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.65 1.675 V. D. Burkert, M. Ripani
E1M711 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.675 1.7 V. D. Burkert, M. Ripani
E1M723 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.7 1.725 V. D. Burkert, M. Ripani
E1M735 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.725 1.75 V. D. Burkert, M. Ripani
E1M746 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.75 1.775 V. D. Burkert, M. Ripani
E1M758 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.775 1.8 V. D. Burkert, M. Ripani
E1M770 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.8 1.825 V. D. Burkert, M. Ripani
E1M782 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.825 1.85 V. D. Burkert, M. Ripani
E1M794 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.85 1.875 V. D. Burkert, M. Ripani
E1M806 dσ/dM(π+,p) e p π+π−p 0.8 1.1 1.875 1.9 V. D. Burkert, M. Ripani
Created in SINP MSU, CLAS Collaboration