ar X iv : h ep - p h / 98 12 27 8 v 2 1 7 D ec 1 99 8 March 2 , 2008 OITS - 667 Determining the Weak Phase γ in the Presence of

ar X iv : h ep - p h / 98 12 27 8 v 1 8 D ec 1 99 8 March 2 , 2008 OITS - 667 Determining the Weak Phase γ in the Presence

We suggest a technique to determine the CKM phase γ without neglecting the soft final state rescattering effects. Using a set of 5 ∆S = 0 (or ∆S = 1) B meson (time integrated) decay rates, we compute the strong phases and magnitudes of the tree and penguin contributions as a function of γ. These are used to predict a ∆S = 1 (∆S = 0) decay rate as a function of γ (using SU (3) symmetry). The mea...

ar X iv : h ep - p h / 98 12 30 2 v 1 9 D ec 1 99 8 Charged right - handed currents in the leptoquark - bilepton flavordynamics chiral models

Flavordynamics chiral models of leptoquark fermions and bilepton gauge bosons with masses up to about 1 TeV, although coincident at low energy with the standard model, address the question of fermion mass hierarchy and explain the flavor question. The presence of charged right-handed weak currents coupled to bileptons, which we point out herein, is another remarkable feature of these chiral the...

ar X iv : h ep - t h / 98 12 18 6 v 1 2 1 D ec 1 99 8 Yangians , finite W - algebras and the Non Linear Schrödinger hierarchy

ar X iv : h ep - t h / 98 12 03 2 v 1 3 D ec 1 99 8 Holography and the Weyl anomaly

We review our calculation of theWeyl anomaly for d-dimensional conformal field theories that have a description in terms of a (d+ 1)-dimensional gravity theory.

ar X iv : h ep - p h / 99 12 28 8 v 2 1 5 D ec 1 99 9 Lattice Calculations and Hadron Physics