10 research outputs found

    "Bare Cross Section" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

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    Bare cross section σbare(e+e−→π+π−(γFSR))\sigma^\mathrm{bare}(e^+e^-\to\pi^+\pi^-(\gamma_\mathrm{FSR})) of the process e+e−→π+π−e^+e^-\to\pi^+\pi^- measured using the initial state radiation method. The data is corrected concerning final state radiation and vacuum polarization effects. The final state radiation is added using the Schwinger term at born level

    "Covariance Matrix of the Pion Form Factor" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

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    Statistical covariance matrix of the pion form factor ∣Fπ∣2|F_\pi|^2

    "Covariance Matrix of the Pion Form Factor" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

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    Statistical covariance matrix of the pion form factor ∣Fπ∣2|F_\pi|^2

    "Pion Form Factor" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

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    Pion form factor ∣Fπ∣2|F_\pi|^2 measured using the initial state radiation method. The data is corrected concerning vacuum polarization effects

    "Pion Form Factor" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

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    Pion form factor ∣Fπ∣2|F_\pi|^2 measured using the initial state radiation method. The data is corrected concerning vacuum polarization effects

    "Table 1" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

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    Results for the bare cross section σπ+π−bare\sigma^\text{bare}_{\pi^+\pi^-} and the pion form factor together with their statistical uncertainties. The systematical uncertainties are given by 0.9% (see arXiv:1507.08188)

    "Bare Cross Section" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

    No full text
    Bare cross section σbare(e+e−→π+π−(γFSR))\sigma^\mathrm{bare}(e^+e^-\to\pi^+\pi^-(\gamma_\mathrm{FSR})) of the process e+e−→π+π−e^+e^-\to\pi^+\pi^- measured using the initial state radiation method. The data is corrected concerning final state radiation and vacuum polarization effects. The final state radiation is added using the Schwinger term at born level

    "Table 1" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

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    Results of the BESIII measurement of the cross section σπ+π−(γFSR)bare≡σbare(e+e−→π+π−(γFSR))\sigma^{\rm bare}_{\pi^+\pi^-(\gamma_{\rm FSR})} \equiv \sigma^{\rm bare}(e^+e^-\rightarrow\pi^+\pi^-(\gamma_{\rm FSR})) and the squared pion form factor ∣Fπ∣2|F_\pi|^2. The errors are statistical only. The value of s′\sqrt{s'} represents the bin center. The 0.9%\% systematic uncertainty is fully correlated between any two bins

    "Covariance Matrix of the Bare Cross Section" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

    No full text
    Statistical covariance matrix of the bare cross section σbare(e+e−→π+π−(γFSR))\sigma^\mathrm{bare}(e^+e^-\to\pi^+\pi^-(\gamma_\mathrm{FSR}))

    "Covariance Matrix of the Bare Cross Section" of "Measurement of the e+e−→π+π−\mathrm e^+\mathrm e^-\rightarrow\mathrm\pi^+\mathrm\pi^- Cross Section between 600 and 900 MeV Using Initial State Radiation"

    No full text
    Statistical covariance matrix of the bare cross section σbare(e+e−→π+π−(γFSR))\sigma^\mathrm{bare}(e^+e^-\to\pi^+\pi^-(\gamma_\mathrm{FSR}))
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