$\phi _{ES}({{\mathit p}{\mathit p}}$)
INSPIRE search
${{\mathit p}}{{\mathit p}}$ solar-neutrino flux measured via ${{\mathit \nu}}{{\mathit e}}$ elastic scattering. This process is sensitive to all active neutrino flavors, but with reduced sensitivity to ${{\mathit \nu}_{{{\mu}}}}$, ${{\mathit \nu}_{{{\tau}}}}$ due to the cross section difference, ${\mathit \sigma (}{{\mathit \nu}}_{{{\mathit \mu}},{{\mathit \tau}}}$ ${{\mathit e}}{)}$ $\sim{}$ 0.3 ${\mathit \sigma (}{{\mathit \nu}_{{{e}}}}{{\mathit e}}{)}$. If the ${{\mathit p}}{{\mathit p}}$ solar-neutrino flux involves nonelectron flavor active neutrinos, their contribution to the flux is $\sim{}$ 0.3 times of ${{\mathit \nu}_{{{e}}}}$.