The observable ϵK is sensitive to flavor violation at some of the highest scales. While its experimental uncertainty is at the half percent level, the theoretical one is in the ballpark of 15%. We explore the nontrivial dependence of the theory prediction and uncertainty on various conventions, like the phase of the kaon fields. In particular, we show how such a rephasing allows to make the short-distance contribution of the box diagram with two charm quarks, ηcc, purely real. Our results allow to slightly reduce the total theoretical uncertainty of ϵK, while increasing the relative impact of the imaginary part of the long distance contribution, underlining the need to compute it reliably. We also give updated bounds on the new physics oper...
International audienceTo quantify the theory error on $R_K$, essentially means to quantify the uncer...
International audienceIn the absence of direct evidence for New Physics at present LHC energies, the...
We calculate the charm quark contribution to the decay K_L -> mu^+ mu^- in next-to-next-to-leading o...
International audienceThe observable ϵ$_{K}$ is sensitive to flavor violation at some of the highest...
The parameter ϵK, that quantifies CP violation in kaon mixing, is the observable setting the stronges...
International audienceThe parameter epsilon_K, that quantifies CP violation in kaon mixing, is the o...
The parameter ε_{K} describes CP violation in the neutral kaon system and is one of the most sensiti...
We present a detailed analysis of ε'/ε within the Standard Model, taking into account the strong enh...
The quantity $\varepsilon'/\varepsilon$ measures direct CP violation in Kaon decays. Recent SM predi...
We propose a method to quantify the Standard Model uncertainty in B → K π decays using the experimen...
We critically review the assumption that no new physics is acting in tree-level B-meson decays and s...
Even if the standard model of particle physics is the most successful quantum field theory ever desi...
Recent theoretical and experimental improvements in the determination of charm and bottom quark mass...
In the Standard Model (SM), the rare transitions where a bottom quark decays into a strange quark an...
The present manuscript describes work pursued in the years 2008-2013 on improving the Standard-Model...
International audienceTo quantify the theory error on $R_K$, essentially means to quantify the uncer...
International audienceIn the absence of direct evidence for New Physics at present LHC energies, the...
We calculate the charm quark contribution to the decay K_L -> mu^+ mu^- in next-to-next-to-leading o...
International audienceThe observable ϵ$_{K}$ is sensitive to flavor violation at some of the highest...
The parameter ϵK, that quantifies CP violation in kaon mixing, is the observable setting the stronges...
International audienceThe parameter epsilon_K, that quantifies CP violation in kaon mixing, is the o...
The parameter ε_{K} describes CP violation in the neutral kaon system and is one of the most sensiti...
We present a detailed analysis of ε'/ε within the Standard Model, taking into account the strong enh...
The quantity $\varepsilon'/\varepsilon$ measures direct CP violation in Kaon decays. Recent SM predi...
We propose a method to quantify the Standard Model uncertainty in B → K π decays using the experimen...
We critically review the assumption that no new physics is acting in tree-level B-meson decays and s...
Even if the standard model of particle physics is the most successful quantum field theory ever desi...
Recent theoretical and experimental improvements in the determination of charm and bottom quark mass...
In the Standard Model (SM), the rare transitions where a bottom quark decays into a strange quark an...
The present manuscript describes work pursued in the years 2008-2013 on improving the Standard-Model...
International audienceTo quantify the theory error on $R_K$, essentially means to quantify the uncer...
International audienceIn the absence of direct evidence for New Physics at present LHC energies, the...
We calculate the charm quark contribution to the decay K_L -> mu^+ mu^- in next-to-next-to-leading o...