The ΔI = 1 2 rule and BK at O(p4) in the chiral expansion
- 16 March 1998
- journal article
- Published by Elsevier in Nuclear Physics B
- Vol. 514 (1-2) , 63-92
- https://doi.org/10.1016/s0550-3213(97)00787-6
Abstract
No abstract availableKeywords
All Related Versions
This publication has 52 references indexed in Scilit:
- IndirectCPviolation in the neutral kaon system beyond leading logarithmsPhysical Review D, 1995
- Enhancement of the KL-KS mass difference by short-distance QCD corrections beyond leading logarithmsNuclear Physics B, 1994
- The ΔS = 1 effective hamiltonian including next-to-leading order QCD and QED correctionsNuclear Physics B, 1994
- The anatomy of ε′/ε beyond leading logarithms with improved hadronic matrix elementsNuclear Physics B, 1993
- Two-loop anomalous dimension matrix for ΔS = 1 weak non-leptonic decays (I). O(α2s)Nuclear Physics B, 1993
- Two-loop anomalous dimension matrix for ΔS = 1 weak non-leptonic decays. (II) O(ααs)Nuclear Physics B, 1993
- ϵ′ϵ at the next-to-leading order in QCD and QEDPhysics Letters B, 1993
- AddendumNuclear Physics B, 1992
- Effective hamiltonians for ΔS = 1 and ΔB = 1 non-leptonic decays beyond the leading logarithmic approximationNuclear Physics B, 1992
- Leading and next-to-leading QCD corrections to ɛ-parameter and B0−¯¯¯B0 mixing in the presence of a heavy top quarkNuclear Physics B, 1990