Abstract

Chiral-scale perturbation theory χχPTσ_σ has been proposed as an alternative to chiral SU(3)L×SU(3)RSU(3)_L\times SU(3)_R perturbation theory which explains the ΔI=1/2ΔI = 1/2 rule for kaon decays. It is based on a low-energy expansion about an infrared fixed point in three-flavor QCD. In χχPTσ_σ, quark condensation ⟨qˉq⟩vac≠0\langle\bar q q \rangle_\mathrm{vac} \neq 0 induces nine Nambu-Goldstone bosons: π,K,ηπ, K, η and a QCD dilaton σσ which we identify with the f0(500)f_0(500) resonance. Partial conservation of the dilatation and chiral currents constrains low-energy constants which enter the effective Lagrangian of χχPTσ_σ. These constraints allow us to obtain new phenomenological bounds on the dilaton decay constant via the coupling of σ/f0σ/f_0 to pions, whose value is known precisely from dispersive analyses of ππππ scattering. Improved predictions for σ→γγσ\to γγ and the σNNσNN coupling are also noted. To test χχPTσ_σ for kaon decays, we revive a 1985 proposal for lattice methods to be applied to K→πK \to π on-shell.

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