We have measured the cross section σ(e+e− →π+π−γ ) at an energy W = mφ = 1.02 GeV with the KLOE detector at the electron–positron collider DAFNE. From the dependence of the cross section on the invariant mass of the two-pion system, we extract σ(e+e− →π+π−) for the mass range 0.35 < s <0.95 GeV^2. From this result, we calculate the pion form factor and the hadronic contribution to the muon anomaly, aμ
We have measured the ratio cr (e(+)e(-) -> pi(+)pi(-)gamma)/sigma(e(+)e(-) -> mu(+)mu(-)gamma), with...
We have measured the cross section σ(e+e −→π+π − γ) with the KLOE detector at DAΦNE, at an energy W ...
The muon anomalous magnetic moment is one of the most precisely measured quantities in particle phys...
We have measured the cross section sigma(e+e -> pi+ pi- gamma) at an energy W = m_phi=1.02 GeV with ...
We have measured the cross section sigma(e(+)e(-) --> pi (+) pi (-) y) at an energy W = m(phi) = 1.0...
We have measured the cross section sigma(e(+)e(-) -> pi(+)pi(-gamma)) at an energy W = m(phi) = 1.02...
We have measured the cross section sigma(e(+)e(-) -> pi(+)pi(-gamma)) at an energy W = m(phi) = 1.02...
We have measured the cross section σ(e+e− → pi+pi−>γ(γ)) at DAΦNE, the Frascati φ–factory, using ...
We have measured the cross section σ(e + e –→π + π – γ) with the KLOE detector at DAΦNE, at an energ...
We have measured the cross section of the radiative process e+e−→π+π−γe+e−→π+π−γ with the KLOE detec...
We have measured the cross section or(e(+)e(-) --> pi(+)pi(-)gamma) as a function of the pi(+)pi(-) ...
We have measured the ratio σ(e+e-→π+π-γ)/σ(e+e-→μ+μ-γ), with the KLOE detector at DAΦNE for a total ...
We have measured the ratio cr (e(+)e(-) -> pi(+)pi(-)gamma)/sigma(e(+)e(-) -> mu(+)mu(-)gamma), with...
We have measured the cross section σ(e+e −→π+π − γ) with the KLOE detector at DAΦNE, at an energy W ...
The muon anomalous magnetic moment is one of the most precisely measured quantities in particle phys...
We have measured the cross section sigma(e+e -> pi+ pi- gamma) at an energy W = m_phi=1.02 GeV with ...
We have measured the cross section sigma(e(+)e(-) --> pi (+) pi (-) y) at an energy W = m(phi) = 1.0...
We have measured the cross section sigma(e(+)e(-) -> pi(+)pi(-gamma)) at an energy W = m(phi) = 1.02...
We have measured the cross section sigma(e(+)e(-) -> pi(+)pi(-gamma)) at an energy W = m(phi) = 1.02...
We have measured the cross section σ(e+e− → pi+pi−>γ(γ)) at DAΦNE, the Frascati φ–factory, using ...
We have measured the cross section σ(e + e –→π + π – γ) with the KLOE detector at DAΦNE, at an energ...
We have measured the cross section of the radiative process e+e−→π+π−γe+e−→π+π−γ with the KLOE detec...
We have measured the cross section or(e(+)e(-) --> pi(+)pi(-)gamma) as a function of the pi(+)pi(-) ...
We have measured the ratio σ(e+e-→π+π-γ)/σ(e+e-→μ+μ-γ), with the KLOE detector at DAΦNE for a total ...
We have measured the ratio cr (e(+)e(-) -> pi(+)pi(-)gamma)/sigma(e(+)e(-) -> mu(+)mu(-)gamma), with...
We have measured the cross section σ(e+e −→π+π − γ) with the KLOE detector at DAΦNE, at an energy W ...
The muon anomalous magnetic moment is one of the most precisely measured quantities in particle phys...