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We have observed the decays B° -» K*(892)°j and B~ -> K*(892)~ry, which are evidence for the quark-level process b -• 57. The average branching fraction is (4.5 ± 1.5 ± 0.9) x 10~5. This value is consistent with standard model predictions from electromagnetic penguin diagrams. PACS numbers: 13.40.Hq, 14.40.Jz One-loop, flavor-changing neutral current diagrams, meson decays [1]. They were later identified as a possible known as penguins, were originally introduced into the source of direct CP violation in kaon decay, and hence as theory of weak decays to explain the AI = \ rule in K a contribution to e! /e [2]. Their importance in B meson 674 0031 -9007/93/71 (5)/674(5)$06.00

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We consider the decay of T(1S) particles produced at CESR into a photon which is observed by the CLEO detector plus particles which are not seen. These could be real particles which fall outside of our acceptance, or particles which are noninteracting. We report the results of our search for the process T(lS) -+ p + "unseen" for photon energies )1 GeV, obtaining limits for the case where "unseen" is either a single particle or a particle-antiparticle pair. Our upper limits represent the highest sensitivity measurements for such decays to date.

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Canada CanadaUsing data collected by the CLEO II detector, we have observed two states decaying to A, +m+R elative to the A, +, their mass splittings are measured to be +307.5~0.4~1.0 and +342.2~0.20 031-9007/95/74(17)/3331(5)$06. 00

A measurement of the cross section for pp -+ pp is performed at two-photon center-of-mass energies between 2.00 and 3.25 GeV. These results are obtained using e+e~e+e pP events selected from 1.31 fb of data taken with the CLEO II detector. The measured cross section *Permanent address: Carleton University, Ottawa, Canada K1S 586.