SU(2) chiral perturbation theory for Kl3 decay amplitudes
arXiv:0809.1229 · doi:10.1016/j.nuclphysb.2008.12.001
Abstract
We use one-loop $\SU(2)_L\times \SU(2)_R$ chiral perturbation theory ($\SU(2)$ ChPT) to study the behaviour of the form-factors for semileptonic decays with the pion mass at and at , where is the momentum transfer. At , the final-state pion has an energy of approximately (for ) and so is not soft, nevertheless it is possible to compute the chiral logarithms, i.e. the corrections of . We envisage that our results at will be useful in extrapolating lattice QCD results to physical masses. A consequence of the Callan-Treiman relation is that in the $\SU(2)$ chiral limit (), the scalar form factor at $\qsqmax$ is equal to , the ratio of the kaon and pion leptonic decay constants in the chiral limit. Lattice results for the scalar form factor at $\qsqmax$ are obtained with excellent precision, but at the masses at which the simulations are performed the results are about 25% below and are increasing only very slowly. We investigate the chiral behaviour of $f^0(\qsqmax)$ and find large corrections which provide a semi-quantitative explanation of the difference between the lattice results and . We stress the generality of the relation $f^0_{P\toπ}(\qsqmax)=f^{(P)}/f$ in the $\SU(2)$ chiral limit, where or and briefly comment on the potential value of using this theorem in obtaining physical results from lattice simulations.
20 pages, 4 figures
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