CLAS Physics Database

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Search results

ID Quantity Beam Target Final state Q2min,
GeV2 		Q2max,
GeV2 		Wmin,
GeV 		Wmax,
GeV 		Spokespersons
E1M4 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.4 1.425 V. D. Burkert, M. Ripani
E1M13 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.425 1.45 V. D. Burkert, M. Ripani
E1M26 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.45 1.475 V. D. Burkert, M. Ripani
E1M36 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.475 1.5 V. D. Burkert, M. Ripani
E1M50 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.5 1.525 V. D. Burkert, M. Ripani
E1M64 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.525 1.55 V. D. Burkert, M. Ripani
E1M72 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.55 1.575 V. D. Burkert, M. Ripani
E1M84 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.575 1.6 V. D. Burkert, M. Ripani
E1M99 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.6 1.625 V. D. Burkert, M. Ripani
E1M110 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.625 1.65 V. D. Burkert, M. Ripani
E1M120 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.65 1.675 V. D. Burkert, M. Ripani
E1M132 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.675 1.7 V. D. Burkert, M. Ripani
E1M147 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.7 1.725 V. D. Burkert, M. Ripani
E1M157 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.725 1.75 V. D. Burkert, M. Ripani
E1M171 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.75 1.775 V. D. Burkert, M. Ripani
E1M183 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.775 1.8 V. D. Burkert, M. Ripani
E1M197 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.8 1.825 V. D. Burkert, M. Ripani
E1M209 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.825 1.85 V. D. Burkert, M. Ripani
E1M219 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.85 1.875 V. D. Burkert, M. Ripani
E1M233 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.875 1.9 V. D. Burkert, M. Ripani
E1M244 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.9 1.925 V. D. Burkert, M. Ripani
E1M254 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.925 1.95 V. D. Burkert, M. Ripani
E1M266 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.95 1.975 V. D. Burkert, M. Ripani
E1M280 dσ/dM(π−,p) e p π+π−p 1.1 1.5 1.975 2.0 V. D. Burkert, M. Ripani
E1M288 dσ/dM(π−,p) e p π+π−p 1.1 1.5 2.0 2.025 V. D. Burkert, M. Ripani
E1M302 dσ/dM(π−,p) e p π+π−p 1.1 1.5 2.025 2.05 V. D. Burkert, M. Ripani
E1M315 dσ/dM(π−,p) e p π+π−p 1.1 1.5 2.05 2.075 V. D. Burkert, M. Ripani
E1M326 dσ/dM(π−,p) e p π+π−p 1.1 1.5 2.075 2.1 V. D. Burkert, M. Ripani
E1M346 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.4 1.425 V. D. Burkert, M. Ripani
E1M348 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.425 1.45 V. D. Burkert, M. Ripani
E1M360 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.45 1.475 V. D. Burkert, M. Ripani
E1M372 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.475 1.5 V. D. Burkert, M. Ripani
E1M385 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.5 1.525 V. D. Burkert, M. Ripani
E1M397 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.525 1.55 V. D. Burkert, M. Ripani
E1M409 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.55 1.575 V. D. Burkert, M. Ripani
E1M420 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.575 1.6 V. D. Burkert, M. Ripani
E1M432 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.6 1.625 V. D. Burkert, M. Ripani
E1M445 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.625 1.65 V. D. Burkert, M. Ripani
E1M457 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.65 1.675 V. D. Burkert, M. Ripani
E1M471 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.675 1.7 V. D. Burkert, M. Ripani
E1M480 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.7 1.725 V. D. Burkert, M. Ripani
E1M492 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.725 1.75 V. D. Burkert, M. Ripani
E1M504 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.75 1.775 V. D. Burkert, M. Ripani
E1M516 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.775 1.8 V. D. Burkert, M. Ripani
E1M528 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.8 1.825 V. D. Burkert, M. Ripani
E1M540 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.825 1.85 V. D. Burkert, M. Ripani
E1M552 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.85 1.875 V. D. Burkert, M. Ripani
E1M564 dσ/dM(π−,p) e p π+π−p 0.5 0.8 1.875 1.9 V. D. Burkert, M. Ripani
E1M576 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.4 1.425 V. D. Burkert, M. Ripani
E1M588 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.425 1.45 V. D. Burkert, M. Ripani
E1M600 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.45 1.475 V. D. Burkert, M. Ripani
E1M612 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.475 1.5 V. D. Burkert, M. Ripani
E1M624 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.5 1.525 V. D. Burkert, M. Ripani
E1M636 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.525 1.55 V. D. Burkert, M. Ripani
E1M648 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.55 1.575 V. D. Burkert, M. Ripani
E1M660 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.575 1.6 V. D. Burkert, M. Ripani
E1M673 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.6 1.625 V. D. Burkert, M. Ripani
E1M685 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.625 1.65 V. D. Burkert, M. Ripani
E1M697 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.65 1.675 V. D. Burkert, M. Ripani
E1M709 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.675 1.7 V. D. Burkert, M. Ripani
E1M721 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.7 1.725 V. D. Burkert, M. Ripani
E1M733 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.725 1.75 V. D. Burkert, M. Ripani
E1M744 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.75 1.775 V. D. Burkert, M. Ripani
E1M756 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.775 1.8 V. D. Burkert, M. Ripani
E1M768 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.8 1.825 V. D. Burkert, M. Ripani
E1M780 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.825 1.85 V. D. Burkert, M. Ripani
E1M792 dσ/dM(π−,p) e p π+π−p 0.8 1.1 1.85 1.875 V. D. Burkert, M. Ripani
E1M804 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