6533b822fe1ef96bd127cca0
RESEARCH PRODUCT
‘‘Improved’’ lattice study of semileptonic decays ofDmesons
N. M. HazelLaurent LellouchD. G. RichardsH. HoeberChristopher T. SachrajdaHartmut WittigK.c. BowlerRichard KenwayJ. Nievessubject
Semileptonic decayPhysicsStatistics::TheoryParticle physicsStatistics::ApplicationsMesonHigh Energy Physics - Lattice (hep-lat)Lattice field theoryZero (complex analysis)Lattice (group)Form factor (quantum field theory)FOS: Physical sciencesFísicaQuenched approximationLattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHigh Energy Physics::Experimentdescription
We present results of a lattice computation of the matrix elements of the vector and axial-vector currents which are relevant for the semi-leptonic decays $D \rightarrow K$ and $D \rightarrow K^*$. The computations are performed in the quenched approximation to lattice QCD on a $24^3 \times 48$ lattice at $\beta=6.2$, using an $O(a)$-improved fermionic action. In the limit of zero lepton masses the semi-leptonic decays $D \rightarrow K$ and $D \rightarrow K^*$ are described by four form factors: $f^{+}_K,V,A_1$ and $A_2$, which are functions of $q^2$, where $q^{\mu}$ is the four-momentum transferred in the process. Our results for these form factors at $q^2=0$ are: $f^+_K(0)=0.67 \er{7}{8}$ , $V(0)=1.01 \err{30}{13}$ , $A_1(0)=0.70 \err{7}{10}$ , $A_2(0)=0.66 \err{10}{15}$ , which are consistent with the most recent experimental world average values. We have also determined the $q^2$ dependence of the form factors, which we find to be reasonably well described by a simple pole-dominance model. Results for other form factors, including those relevant to the decays \dpi and \drho, are also given.
year | journal | country | edition | language |
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1995-05-01 | Physical Review D |