Connecting the Quenched and Unquenched Worlds via the Large N_c World
arXiv:hep-lat/0205014 · doi:10.1016/S0370-2693(02)02461-9
Abstract
In the large N_c(number of colors) limit, quenched QCD and QCD are identical. This implies that, in the effective field theory framework, some of the low energy constants in (N_c=3) quenched QCD and QCD are the same up to higher-order corrections in the 1/N_c expansion. Thus the calculation of the nonleptonic kaon decays relevant for the Delta I=1/2 rule in the quenched approximation is expected to differ from the unquenched one by an O(1/N_c) correction. However, the calculation relevant to the CP-violation parameter epsilon'/epsilon would have a relatively big higher-order correction due to the large cancellation in the leading order. Some important weak matrix elements are poorly known that even constraints with 100% errors are interesting. In those cases, quenched calculations will be very useful.
8 pages, one figure; minor typos corrected
References in corpus (9)
- MRST2001: partons and alpha_S from precise deep inelastic scattering and Tevatron jet data
- NNLO global parton analysis
- Partially quenched chiral perturbation theory without
- Heavy quark physics from lattice QCD
- The Magnetic Moments of the Octet Baryons in Quenched Chiral Perturbation Theory
- Parity Violating Photoproduction of on the Resonance
- Parity-Violating Pion-Nucleon Coupling h_{πNN}^{(1)} from π^+ Electroproton Production Near the Threshold
- Physical Results from Partially Quenched Simulation
- Heavy-light decay constants with three dynamical flavors
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- The Chiral Extrapolation of Strange Matrix Elements in the Nucleon
- Generalised parton distributions of the pion in partially-quenched chiral perturbation theory
- Topics in Effective Field Theory for Lattice QCD