17 research outputs found
Evidence for Factorization in Three-body Decays
Motivated by experimental results on , we use a
factorization approach to study these decays. Two mechanisms concerning kaon
pair production arise: current-produced (from vacuum) and transition (from the
meson). The kaon pair in the decays can be
produced only by the vector current (current-produced), whose matrix element
can be extracted from processes via isospin relations. The
decay rates obtained this way are in good agreement with experiment. The
decays involve both current-produced and transition
processes. By using QCD counting rules and the measured decay rates, the measured decay spectra can be understood.Comment: 3 pages, 6 figures. Talk presented at EPS2003 Conference, Aachen,
Germany, July 200
Charmed weak decays into in the light-front quark model
More than ten weak decay modes have been measured with the
branching fractions relative to that of . In order
to extract the absolute branching fractions, the study of
is needed. In this work, we predict
with the transition form factors calculated in the
light-front quark model. We also predict and .
The previous values for have been found to deviate
from the most recent observation. Nonetheless, our is able to alleviate the deviation. Moreover, we obtain
, which is consistent with the current
data.Comment: 12 pages, 2 figure
Possible Hints and Search for Glueball Production in Charmless Rare B Decays
Recent data on B->p pbar K, K0 pi pi and K Kbar K hint at a GeV
object recoiling against a kaon. This could be the narrow state observed in
J/\psi -> gamma xi. Nonobservation in p pbar annihilation implies few , consistent with eta_c and J/\psi
decays, but there are actual hints in p pbar -> phi phi and p p-> p pi^+ pi^-
pi^+ pi^- p. Simple modeling shows , appearing as a spike in the spectrum, with
30 events per 100 fb; modes such as K K_s K_s, K phi phi, K4 pi
(K f_2 pi pi) etc. should be explored. The underlying dynamics of g* -> g xi is
analogous to g* -> g etaprime or gluon fragmentation. Discovery of sizable B ->
xi K could be useful for CP violation studies.Comment: 4 pages, 3 figure
Prediction of Three-body Decay Rates
We predict the rates of the charmless three-body and
modes due to weak vector current contributions to be and , respectively. The basis is a
factorization approach of current produced nucleon pairs, together with an
isospin transformation that relates nucleon weak vector form factors to
electromagnetic form factors. Adding the axial vector current contribution, we
find and to be at
order. The three-body modes appear to dominate over the two-body modes such as
, .Comment: 5 pages, 4 figures. Version to appear in Phys. Lett.
Charmless Three-Body Baryonic B Decays
Motivated by recent data on B-> p pbar K decay, we study various charmless
three-body baryonic B decay modes, including Lambda pbar pi, Sigma0 pbar pi, p
pbar pi, p pbar Kbar0, in a factorization approach. These modes have rates of
order 10^{-6}. There are two mechanisms for the baryon pair production,
current-produced and transition. The behavior of decay spectra from these
baryon production mechanisms can be understood by using QCD counting rules.
Predictions on rates and decay spectra can be checked in the near future.Comment: 26 pages, 9 figures; version to appear in Phys. Rev.
Evidence for Factorization in Three-body B --> D(*) K- K0 Decays
Motivated by recent experimental results, we use a factorization approach to
study the three-body B --> D(*) K- K0 decay modes. Two mechanisms are proposed
for kaon pair production: current-produced (from vacuum) and transition (from B
meson). The Bbar0 --> D(*)+ K- K0 decay is governed solely by the
current-produced mechanism. As the kaon pair can be produced only by the vector
current, the matrix element can be extracted from e+ e- --> K Kbar processes
via isospin relations. The decay rates obtained this way are in good agreement
with experiment. Both current-produced and transition processes contribute to
B- --> D(*)0 K- K0 decays. By using QCD counting rules and the measured B- -->
D(*)0 K- K0 decay rates, the measured decay spectra can be understood.Comment: 17 pages, 6 figure