We have measured the cross section of the radiative process e(+)e(-) -> pi(+)pi(-)gamma with the KLOE detector at the Frascati phi-factory DA(1)NE, from events taken at a CM energy W =1 GeV. Initial state radiation allows us to obtain the cross section for e(+)e(-) -> pi(+)pi(-), the pion form factor vertical bar F-pi vertical bar(2) and the dipion contribution to the muon magnetic moment anomaly, Delta alpha(pi pi)(mu) = (478.5 +/- 2.0(stat) +/- 5.0(syst) +/- 4.5(th)) x 10(-10) in the range 0.1 < M-pi pi(2) <0.85 GeV2, where the theoretical error includes a SU(3) chi PT estimate of the uncertainty on photon radiation from the final pions. The discrepancy between the Standard Model evaluation of alpha(mu) and the value measured by the Muon ...
We have measured the cross section or(e(+)e(-) --> pi(+)pi(-)gamma) as a function of the pi(+)pi(-) ...
We have measured the ratio cr (e(+)e(-) -> pi(+)pi(-)gamma)/sigma(e(+)e(-) -> mu(+)mu(-)gamma), with...
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 of the radiative process e(+)e(-) -> pi(+)pi(-)gamma with the KLO...
"We have measured the cross section of the radiative process e(+)e(-) -> pi(+)pi(-)gamma with the KL...
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 sigma(e(+)e(-) -> pi(+)pi(-)gamma(gamma)) at DA Phi NE, the Frasc...
We have measured the cross section sigma(e(+)e(-) -> pi(+)pi(-)gamma(gamma)) at DA Phi NE, the Frasc...
We have measured the cross section σ(e+e− → pi+pi−>γ(γ)) at DAΦNE, the Frascati φ–factory, using ...
AbstractWe have measured the cross section of the radiative process e+e−→π+π−γ with the KLOE detecto...
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 (-) 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 or(e(+)e(-) --> pi(+)pi(-)gamma) as a function of the pi(+)pi(-) ...
We have measured the ratio cr (e(+)e(-) -> pi(+)pi(-)gamma)/sigma(e(+)e(-) -> mu(+)mu(-)gamma), with...
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 of the radiative process e(+)e(-) -> pi(+)pi(-)gamma with the KLO...
"We have measured the cross section of the radiative process e(+)e(-) -> pi(+)pi(-)gamma with the KL...
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 sigma(e(+)e(-) -> pi(+)pi(-)gamma(gamma)) at DA Phi NE, the Frasc...
We have measured the cross section sigma(e(+)e(-) -> pi(+)pi(-)gamma(gamma)) at DA Phi NE, the Frasc...
We have measured the cross section σ(e+e− → pi+pi−>γ(γ)) at DAΦNE, the Frascati φ–factory, using ...
AbstractWe have measured the cross section of the radiative process e+e−→π+π−γ with the KLOE detecto...
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 (-) 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 or(e(+)e(-) --> pi(+)pi(-)gamma) as a function of the pi(+)pi(-) ...
We have measured the ratio cr (e(+)e(-) -> pi(+)pi(-)gamma)/sigma(e(+)e(-) -> mu(+)mu(-)gamma), with...
We have measured the cross section sigma(e+e -> pi+ pi- gamma) at an energy W = m_phi=1.02 GeV with ...