12 research outputs found
Precision Measurements of the Charged Pion, Charged Kaon, and Proton Electromagnetic Form Factors at s = 13.48 GeV^2
Using 20.7 pb^-1 of e+e- annihilation data taken at sqrt{s} = 3.671 GeV with
the CLEO-c detector, precision measurements of the electromagnetic form factors
of the charged pion, charged kaon, and proton have been made for timelike
momentum transfers of |Q^2| = 13.48 GeV^2 by the reaction e+e- -> h+h-. The
measurements are the first ever with identified pions and kaons of |Q^2| > 4
GeV^2, with the results |F_pi(13.48 GeV^2)| = 0.075 +- 0.008(stat) +-
0.005(syst) and |F_K(13.48 GeV^2)| = 0.063 +- 0.004(stat) +- 0.001(syst). The
result for the proton, assuming |G^p_E| = |G^p_M|, is |G^p_M(13.48 GeV^2)| =
0.014 +- 0.002(stat) +- 0.001(syst), which is in agreement with earlier
results.Comment: 3 pages, 2 figures, contributed to PANIC0
Charm Input for Determining gamma/phi_3
Overconstraining the CKM unitarity triangle with precision measurements of
its angles continues to test the validity of the Standard Model. One of these
angles, gamma/phi_3, has been measured by studying B+- -> D K+- decays, where D
= D0 or D0-bar. I present recent results of hadronic D decays which will
improve the sensitivity of gamma/phi_3 measurements.Comment: 4 pages, CIPANP 2009 proceedings; references adde
Charm Factories: Present and Future
The next generation tau-charm factory, the third Beijing Electron
Spectrometer (BESIII) at the new Beijing Electron Positron Collider (BEPCII),
has begun data collection. I discuss the flavor physics reach of the BESIII
charm program and conclude with a discussion on future proposed tau-charm
facilities.Comment: 4 pages, CIPANP 2009 proceeding
Search for X(3872) in gamma gamma Fusion and ISR at CLEO
We report on a search for the X(3872) state using 15.1 fb^{-1} of e+ e-
annihilation data taken with the CLEO III detector in the sqrt{s} = 9.46-11.30
GeV region. Separate searches for the production of X(3872) in untagged gamma
gamma fusion and e+ e- annihilation following initial state radiation are made
by taking advantage of the unique correlation of J/psi -> l+ l- in X(3872)
decay into J/psi pi+ pi-. No signals are observed in either case, and 90%
confidence upper limits are established as (2J+1)Gamma_{gammagamma}(X(3872))B(X
-> J/psi pi+ pi-) J/psi pi+ pi-) < 8.3
eV.Comment: 4 pages, 2 figures, to appear in the proceedings of the 1st Meeting
of the APS Topical Group on Hadronic Physics, Fermilab, Oct. 24-26, 200