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The KLOE experiment at the $\phi-factory$ DA$\Phi$NE in Frascati is the first to have employed Initial State Radiation (ISR) to precisely determine the $e^+e^-\to\pi^+\pi^-(\gamma)$ cross section below 1 GeV. Such a measurement is…

High Energy Physics - Experiment · Physics 2018-02-14 Graziano Venanzoni

The measurement of the $\sigma(e^+e^-\rightarrow \pi^+\pi^-)$ cross section allows to determine the pion form factor $| F_\pi |^2$ and the two pion contribution to the muon anomaly $a_\mu$. Such a measurement has been performed with the…

High Energy Physics - Experiment · Physics 2019-08-14 Veronica De Leo

In the fixed energy environment of the $e^{+}e^{-}$ collider DA$\Phi$NE, KLOE can measure the cross section of the process $e^{+}e^{-} \to hadrons$ as a function of the hadronic system energy using the radiative return method. At energies…

High Energy Physics - Experiment · Physics 2012-08-03 The KLOE Collaboration , B. Valeriani

The KLOE Experiment at the $\phi$ factory DA$\Phi$NE, has measured the cross section $\sigma(e^+e^-\to\pi^+\pi^-\gamma)$ using two different selection schemes: requiring the photon emission at small polar angle and detecting the photon at…

High Energy Physics - Experiment · Physics 2012-08-27 The KLOE Collaboration

We present a study of the reaction e+e- \to pi+pi-gamma at the phi peak with the KLOE detector at the phi-factory DAPHNE. This reaction allows us to obtain the cross section for \e+e- \to pi+pi- from the e+e- center-of-mass energy W =…

High Energy Physics - Experiment · Physics 2012-08-27 The KLOE Collaboration

In the fixed energy environment of the $e^{+}e^{-}$ collider DA$\Phi$NE, KLOE can measure the cross section of the process $e^{+}e^{-} \to$ hadrons as a function of the hadronic system energy using the radiative return. At energies below 1…

High Energy Physics - Experiment · Physics 2009-05-18 The KLOE Collaboration , presented by G. Venanzoni

We report on the measurement of the hadronic cross section below 1GeV at the electron-positron-collider DAPHNE, using the multiple purpose detector KLOE. The radiative return, which is due to initial state radiation (e+ e- \to gamma +…

High Energy Physics - Experiment · Physics 2010-05-28 The KLOE collaboration , presented by Achim Denig

As a future upgrade of the Frascati phi factory DAPHNE an increase of the center-of-mass energy of the accelerator up to W=2GeV has been proposed (DAFNE2). In this case the hadronic cross section in the energy range between 1-2 GeV can be…

High Energy Physics - Experiment · Physics 2009-05-18 Achim G. Denig , KLOE Collaboration

We have measured the cross section of the radiative process e+e- -> pi+pi-gamma with the KLOE detector at the Frascati phi-factory DAPHNE, from events taken at a CM energy W=1 GeV. Initial state radiation allows us to obtain the cross…

We have measured the cross section $\sigma(e^+e^-\to\pi^+\pi^-\gamma(\gamma))$ at DA$\Phi$NE, the Frascati \phi-factory, using events with initial state radiation photons emitted at small angle and inclusive of final state radiation. We…

High Energy Physics - Experiment · Physics 2012-08-27 KLOE Collaboration

We have measured the cross section $\sigma(e^+e^-\to\pi^+\pi^-\gamma)$ with the KLOE detector at DA$\Phi$NE, at an energy $W=M_\phi=1.02$ GeV. From the dependence of the cross section on $m(\pi^+\pi^-)=\sqrt{W^2-2WE_\gamma}$, where…

High Energy Physics - Experiment · Physics 2008-11-26 The KLOE Collaboration , A. Aloisio

We have measured the cross section $\sigma(e^+e^-\to \pi^+\pi^- \gamma)$ at an energy $W=m_\phi=1.02$ GeV with the KLOE detector at the electron-positron collider DA$\Phi$NE. From the dependence of the cross section on the invariant mass of…

High Energy Physics - Experiment · Physics 2008-11-26 The KLOE Collaboration , A. Aloisio

We have measured the cross section sigma(e+e- \to pi+pi-gamma) as a function of the pi+pi- invariant mass, M_pipi, with the KLOE detector at DAPHNE (W=m_phi=1.02GeV). The photon in the above process is due to Initial State Radiation.…

High Energy Physics - Experiment · Physics 2007-05-23 Achim Denig , KLOE collaboration

Recently it has been demonstrated that particle factories, such as DAPHNE and PEP-II, operating at fixed center-of-mass energies, are able to measure hadronic cross sections as a function of the hadronic system energy using the raditive…

High Energy Physics - Experiment · Physics 2019-08-14 Achim G. Denig

The KLOE experiment at the DA$\Phi$NE $\phi$-factory has performed a new precise measurement of the pion form factor using Initial State Radiation events. Results based on an integrated luminosity of 240 pb$^{-1}$ and extraction of the…

High Energy Physics - Experiment · Physics 2019-08-13 Paolo Beltrame

This document reviews the physics program of the KLOE-2 detector at DA$\Phi$NE upgraded in energy and provides a simple solution to run the collider above the $\phi$-peak (up to 2, possibly 2.5 GeV). It is shown how a precise measurement of…

High Energy Physics - Experiment · Physics 2010-07-30 D. Babusci , C. Bini , F. Bossi , G. Isidori , D. Moricciani , F. Nguyen , P. Raimondi , G. Venanzoni , D. Alesini , F. Archilli , D. Badoni , R. Baldini-Ferroli , M. Bellaveglia , G. Bencivenni , M. Bertani , M. Biagini , C. Biscari , C. Bloise , V. Bocci , R. Boni , M. Boscolo , P. Branchini , A. Budano , S. A. Bulychjev , B. Buonomo , P. Campana , G. Capon , M. Castellano , F. Ceradini , E. Chiadroni , P. Ciambrone , L. Cultrera , E. Czerwinski , E. Dané , G. Delle Monache , E. De Lucia , T. Demma , G. De Robertis , A. De Santis , G. De Zorzi , A. Di Domenico , C. Di Donato , B. Di Micco , E. Di Pasquale , G. Di Pirro , R. Di Salvo , D. Domenici , A. Drago , M. Esposito , O. Erriquez , G. Felici , M. Ferrario , L. Ficcadenti , D. Filippetto , S. Fiore , P. Franzini , G. Franzini , A. Gallo , G. Gatti , P. Gauzzi , S. Giovannella , A. Ghigo , F. Gonnella , E. Graziani , S. Guiducci , F. Happacher , B. Höistad , E. Iarocci , M. Jacewicz , T. Johansson , W. Kluge , V. V. Kulikov , A. Kupsc , J. Lee Franzini , C. Ligi , F. Loddo , P. Lukin , F. Marcellini , C. Marchetti , M. A. Martemianov , M. Martini , M. A. Matsyuk , G. Mazzitelli , R. Messi , C. Milardi , M. Mirazzita , S. Miscetti , G. Morello , P. Moskal , S. Müeller , S. Pacetti , G. Pancheri , E. Pasqualucci , M. Passera , A. Passeri , V. Patera , A. D. Polosa , M. Preger , L. Quintieri , A. Ranieri , P. Rossi , C. Sanelli , P. Santangelo , I. Sarra , M. Schioppa , B. Sciascia , M. Serio , F. Sgamma , M. Silarski , B. Spataro , A. Stecchi , A. Stella , S. Stucci , C. Taccini , S. Tomassini , L. Tortora , C. Vaccarezza , R. Versaci , W. Wislicki , M. Wolke , J. Zdebik , M. Zobov
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