0000000000882169

AUTHOR

C.r. Allton

showing 2 related works from this author

B-parameters for ΔS=2 supersymmetric operators

1998

We present a calculation of the matrix elements of the most general set of DeltaS=2 dimension-six four-fermion operators. The values of the matrix elements are given in terms of the corresponding B-parameters. Our results can be used in many phenomenological applications, since the operators considered here give important contributions to K^0--K^0bar mixing in several extensions of the Standard Model (supersymmetry, left-right symmetric models, multi-Higgs models etc.). The determination of the matrix elements improves the accuracy of the phenomenological analyses intended to put bounds on basic parameters of the different models, as for example the pattern of the sfermion mass matrices. Th…

DeltaNuclear and High Energy PhysicsHigh Energy Physics::LatticeLattice (group)FOS: Physical sciencesQuenched approximationRenormalizationMatrix (mathematics)Theoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)Mixing (physics)Mathematical physicskaon decays lattice supersymmetryPhysicsHigh Energy Physics - Lattice (hep-lat)FísicaSupersymmetryAtomic and Molecular Physics and Opticskaone decays lattice supersymmetryFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)SfermionNon-perturbative
researchProduct

Semi-leptonic Decays of Heavy Flavours on a Fine Grained Lattice

1994

We present the results of a numerical calculation of semi-leptonic form factors relevant for heavy flavour meson decays into light mesons, at $\beta=6.4$ on a $24^3 \times 60$ lattice, using the Wilson action in the quenched approximation. We obtain $f^+_K(0)=0.65\pm 0.18$, $V(0)=0.95\pm 0.34$, $A_1(0)=0.63\pm 0.14 $ and $A_2(0)=0.45\pm 0.33 $. We also obtain $A_1(q^2_{max})=0.62\pm 0.09$, $V(0)/A_1(0)=1.5\pm 0.28 $ and $A_2(0)/A_1(0)=0.7\pm 0.4$. The results for $f^+_K(0)$, $V(0)$ and $A_1(0)$ are consistent with the experimental data and with previous lattice determinations with larger lattice spacings. In the case of $A_2(0)$ the errors are too large to draw any firm conclusion. We have …

QuarkPhysicsNuclear and High Energy PhysicsFirm conclusionParticle physicsMesonHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesQuenched approximationHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)Heavy quark effective theoryB meson
researchProduct