Add to ORKGWe have previously analysed the chiral predictions for the decay KL ! 0 e+e− and discussed how experimental measurements of this process can help our understanding of chiral theories and of CP tests. Motivated by the possibility that the analogous muonic process may soon be measurable, we extend this calculation to the decay KL ! 0 μ+μ−. Branching ratios and differential branching ratios are calculated and presented. Measurements of these will help shed some light on the puzzles in our understanding of the chiral loop effects which were raised by the rate for KL ! 0
The decay rate of KL → π0 γ γ has been measured with the NA48 detector at the CERN SPS. A total of 2...
The decay rate of KL \u2192 \u3c00 \u3b3 \u3b3 has been measured with the NA48 detector at the CERN ...
With the E731 apparatus at Fermilab, we have simultaneously collected 6859 K(L) and K(S) decays into...
The decay KL→π0γe+e- occurs at a higher rate than the nonradiative process KL→π0e+e-, and hence can ...
Agreement between the experimental value Γ(KS→γγ) and the number predicted via a one-loop chiral per...
The KTeV experiment has carried out a broad program of studies of rare kaon decays. In this paper we...
The decay KL→π0e+e- is searched for as a signal of direct ΔS=1 CP violation. We provide a thorough u...
Data from NA31 experiment at CERN have been used to measure the decay KS → γγ. From 69 candidate eve...
We review some new developments in the theoretical description of the processes K ->pi gamma gamma, ...
The increasing body of experimental data motivates us to investigate a new contribution to the radia...
Data from NA31 experiment at CERN have been used to measure the decay KS → γγ. From 69 candidate eve...
The increasing body of experimental data motivates us to investigate a new contribution to the radia...
The increasing body of experimental data motivates us to investigate a new contribution to the radia...
The increasing body of experimental data motivates us to investigate a new contribution to the radia...
The π0→γγ decay width is analyzed within the combined framework of chiral perturbation theory and th...
The decay rate of KL → π0 γ γ has been measured with the NA48 detector at the CERN SPS. A total of 2...
The decay rate of KL \u2192 \u3c00 \u3b3 \u3b3 has been measured with the NA48 detector at the CERN ...
With the E731 apparatus at Fermilab, we have simultaneously collected 6859 K(L) and K(S) decays into...
The decay KL→π0γe+e- occurs at a higher rate than the nonradiative process KL→π0e+e-, and hence can ...
Agreement between the experimental value Γ(KS→γγ) and the number predicted via a one-loop chiral per...
The KTeV experiment has carried out a broad program of studies of rare kaon decays. In this paper we...
The decay KL→π0e+e- is searched for as a signal of direct ΔS=1 CP violation. We provide a thorough u...
Data from NA31 experiment at CERN have been used to measure the decay KS → γγ. From 69 candidate eve...
We review some new developments in the theoretical description of the processes K ->pi gamma gamma, ...
The increasing body of experimental data motivates us to investigate a new contribution to the radia...
Data from NA31 experiment at CERN have been used to measure the decay KS → γγ. From 69 candidate eve...
The increasing body of experimental data motivates us to investigate a new contribution to the radia...
The increasing body of experimental data motivates us to investigate a new contribution to the radia...
The increasing body of experimental data motivates us to investigate a new contribution to the radia...
The π0→γγ decay width is analyzed within the combined framework of chiral perturbation theory and th...
The decay rate of KL → π0 γ γ has been measured with the NA48 detector at the CERN SPS. A total of 2...
The decay rate of KL \u2192 \u3c00 \u3b3 \u3b3 has been measured with the NA48 detector at the CERN ...
With the E731 apparatus at Fermilab, we have simultaneously collected 6859 K(L) and K(S) decays into...