Observation of {psi}(3770){yields}{gamma}{chi}{sub c1}{yields}{gamma}{gamma}J/{psi}

From e{sup +}e{sup -} collision data acquired with the CLEO detector at the Cornell Electron Storage Ring, we observe the non-DD decay {psi}(3770){yields}{gamma}{chi}{sub c1} with a statistical significance of 6.6 standard deviations, using the two-photon cascades to J/{psi} and J/{psi}{yields}l{sup...

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Veröffentlicht in:Physical review letters 2006-05, Vol.96 (18)
Hauptverfasser: Coan, T.E., Gao, Y.S., Liu, F., Artuso, M., Boulahouache, C., Blusk, S., Butt, J., Dorjkhaidav, O., Li, J., Menaa, N., Mountain, R., Nandakumar, R., Randrianarivony, K., Redjimi, R., Sia, R., Skwarnicki, T., Stone, S., Wang, J. C., Zhang, K., Csorna, S. E.
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Sprache:eng
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Zusammenfassung:From e{sup +}e{sup -} collision data acquired with the CLEO detector at the Cornell Electron Storage Ring, we observe the non-DD decay {psi}(3770){yields}{gamma}{chi}{sub c1} with a statistical significance of 6.6 standard deviations, using the two-photon cascades to J/{psi} and J/{psi}{yields}l{sup +}l{sup -}. We determine {sigma}(e{sup +}e{sup -}{yields}{psi}(3770))xB({psi}(3770){yields}{gamma}{chi}{sub c1})=(18.0{+-}3.3= {+-}2.5) pb and branching fraction B({psi}(3770){yields}{gamma}{chi}{sub c1})=(2.8{+-}0.5{+-}0.4)x10{sup -3}. We set 90% C.L. upper limits for the transition to {chi}{sub c2} ({chi}{sub c0}): {sigma}xB
ISSN:0031-9007
1079-7114
DOI:10.1103/PhysRevLett.96.182002