216 research outputs found
Measurements of Lifetimes and a Limit on the Lifetime Difference in the Neutral D-Meson System
Using the large hadroproduced charm sample collected in experiment E791 at
Fermilab, we report the first directly measured constraint on the decay-width
difference Delta Gamma for the mass eigenstates of the D0-D0bar system. We
obtain our result from lifetime measurements of the decays D0 --> K-pi+ and D0
--> K-K+, under the assumption of CP invariance, which implies that the CP
eigenstates and the mass eigenstates are the same. The lifetime of D0 --> K-K+
(the CP-even final state is \tau_KK = 0.410 +/- 0.011 +/- 0.006 ps, and the
lifetime of D0 --> K-pi+ (an equal mixture of CP-odd and CP-even final states
is tau_Kpi = 0.413 +/- 0.003 +/- 0.004 ps. The decay-width difference is Delta
Gamma = 2(Gamma_KK - Gamma_Kpi) = 0.04 +/- 0.14 +/- 0.05 ps^-1. We relate these
measurements to measurements of mixing in the neutral D-meson system.Comment: 8 pages + 3 figures + 2 table
Measurement of the K-pi+ S-wave System in D+ to K-pi+pi+ Decays from Fermilab E791
A new approach to the analysis of three body decays is presented.
Measurements of the S-wave K pi amplitude are made in independent ranges of
invariant mass from threshold up to the upper kinematic limit in D+ to K-pi+pi+
decays. These are compared with results obtained from a fit where the S-wave is
assumed to have kappa(800) and K*0(1430) resonances. Results are also compared
with measurements of K-pi+ elastic scattering. Contributions from I = 1/2 and I
= 3/2 are not resolved in this study. If I = 1/2 dominates, however, the Watson
theorem prediction, that the phase behavour below K-eta' threshold should match
that in elastic scattering, is not well supported by these data. Production of
K-pi+ from these D decays is also studied.Comment: Submitted to International Conference on Hadron Spectroscopy, Rio de
Janeiro, August (2005
Color Transparency via Coherent Exclusive rho Production
We examine the potential of the COMPASS experiment at CERN to study color
transparency via exclusive coherent vector meson production in hard
muon-nucleus scattering. It is demonstrated that COMPASS has high sensitivity
to test this important prediction of perturbative QCD.Comment: Feasibility study for COMPASS collaboration, 3 pages, no figures, 1
table. This contribution is based on talk presented at the Workshop on Spin
Physics, Trento, Italy, July 2001. The conference www site is
http://ECTstar.ect.it/contents.html The proceedings of the workshop will be
published as a special issue of Nuclear Physics B (proc suppl), eds. S Bass,
A De Roeck and A Deshpande. A more complete 26 page feasibility study with 7
figures and 3 tables is available as A. Sandacz et al., hep-ex/0106076
Revision of 26 Sept. for Ref. 11 modificatio
The Leading Particle Effect from Heavy-Quark Recombination
The leading particle effect in charm hadroproduction is an enhancement of the
cross section for a charmed hadron D in the forward direction of the beam when
the beam hadron has a valence parton in common with the D. The large D+/D-
asymmetry observed by the E791 experiment is an example of this phenomenon. We
show that the heavy-quark recombination mechanism provides an economical
explanation for this effect. In particular, the D+/D- asymmetry can be fit
reasonably well using a single parameter whose value is consistent with a
recent determination from charm photoproduction.Comment: Revtex file, 4 pages, 3 figure
QCD sum rule approach for the light scalar mesons as four-quark states
We study the two point-function for the scalar mesons and as diquak-antidiquark states. We also study the decays
of these mesons into , and . We found that the
couplings are consistent with existing experimental data, pointing in favor of
the four-quark structure for the light scalar mesons.Comment: 6 pages, 4 figure
Coulomb induced diffraction of energetic hadrons into jets
The electromagnetic (e.m.) current conservation and renormalizability of QCD
are used to calculate the amplitude of energetic hadron(photon) diffraction
into several jets with large relative transverse momenta off the
nucleon(nucleus) Coulomb field. Numerical estimates of the ratio of e.m. and
strong amplitudes show that within the kinematic range where the leading twist
approximation for the strong amplitude is applicable, the e.m. contribution can
be neglected. In pA scattering at LHC and in the fragmentation of a photon into
two jets in ultraperipheral AA collisions in the black limit (which maybe
realistic at LHC) e.m. contribution may win.Comment: 10 page
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