2001/01/19 by J. O. Eeg, Svjetlana Fajfer, S. Fajfer +2 · 2 citations
Physics and Astronomy · #High-Energy Particle Collisions Research #Particle physics theoretical and experimental studies #Quantum Chromodynamics and Particle Interactions #hep-ph
paper · pdf · doi:10.1103/physrevd.64.034010
published as Phys.Rev. D64 (2001) 034010 · 20 pages, 8 figures
arxiv created 2001/01/19 · openalex publication_date 2001/07/03 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/28
We point out that the decay mode D0\ensuremath→K0K0 has no factorizable contribution. In chiral perturbation language, treating D0 as heavy, the O(p) contribution is zero. We calculate the nonfactorizable chiral loop contributions of order O(p3). Then, we use a heavy-light type chiral quark model to calculate nonfactorizable tree level terms, also of order O(p3), proportional to the gluon condensate. A priori, chiral loops are not expected to give good precision because the energy release in this decay is almost 800 MeV. Still, we find that both the chiral loops and the gluon condensate contributions are of the same order of magnitude as the experimental amplitude.