Spectator scattering at NLO in non-leptonic B decays: Leading penguin amplitudes
نویسنده
چکیده
We complete the computation of the 1-loop (αs) corrections to hard spectator scattering in non-leptonic B decays at leading power in Λ/mb by evaluating the penguin amplitudes. This extends the knowledge of these next-to-next-to-leadingorder contributions in the QCD factorization formula for B decays to a much wider class of final states, including all pseudoscalar-pseudoscalar, pseudoscalar-vector, and longitudinally polarized vector-vector final states, except final states with η or η′ mesons. The new 1-loop correction is significant for the colour-suppressed amplitudes, but turns out to be strongly suppressed for the leading QCD penguin amplitude αp4. We provide numerical values of the phenomenological P/T and C/T amplitude ratios for the ππ, πρ and ρρ final states, and discuss corrections to several relations between electroweak penguin and tree amplitudes. Address after 01 October 2006: Arnold Sommerfeld Center, Department für Physik, LudwigMaximilians-Universität München, Theresienstraße 37, D-80333 München, Germany
منابع مشابه
Penguin Amplitudes in Hadronic B Decays: Nlo Spectator Scattering
We present results on the NLO (α2s) spectator-scattering corrections to the topological penguin amplitudes for charmless hadronic two-body B-decays in QCD factorization. The corrections can be sizable for the colour-suppressed electroweak penguin amplitudes α 4,EW but otherwise are numerically small. Our results explicitly demonstrate factorization at this order. To assess the phenomenological ...
متن کاملRadiative corrections to hard spectator scattering in B → ππ decays
We present the calculation of the next-to-leading corrections to the tree amplitudes which appear in the description of non-leptonic B-decays in the factorization approach. These corrections, together with radiative corrections to the jet functions, represent the full next-to-leading contributions to the dominant hard spectator scattering term generated by operators O1,2 in the decay amplitudes...
متن کاملElectroweak Penguin Contributions to Non - Leptonic ∆ F = 1 Decays at NNLO
We calculate the O(αs) corrections to the Z-penguin and electroweak box diagrams relevant for non-leptonic ∆F = 1 decays with F = S,B. This calculation provides the complete O(αWαs) and O(αWαs sin θWmt ) corrections (αW = α/ sin θW ) to the Wilson coefficients of the electroweak penguin four quark operators relevant for non-leptonic Kand B-decays. We argue that this is the dominant part of the ...
متن کامل4 Radiative B decays to the axial K mesons at next - to - leading order Jong - Phil
We calculate the branching ratios of B → K1γ at next-to-leading order (NLO) of αs where K1 is the orbitally excited axial vector meson. The NLO decay amplitude is divided into the vertex correction and the hard spectator interaction part. The one is proportional to the weak form factor of B → K1 transition while the other is a convolution between light-cone distribution amplitudes and hard scat...
متن کاملRadiative B decays to the axial K mesons at next - to - leading order
We calculate the branching ratios of B → K1γ at next-to-leading order (NLO) of αs where K1 is the orbitally excited axial vector meson. The NLO decay amplitude is divided into the vertex correction and the hard spectator interaction part. The one is proportional to the weak form factor of B → K1 transition while the other is a convolution between light-cone distribution amplitudes and hard scat...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 2007