Abstract

If heavy neutrinos with mass mνH≥m_{ν_{H}}\geq2me m_e are produced in the Sun via the decay 8B→8Be+e++νH{^8\rm{B}} \rightarrow {^8\rm{Be}} + e^+ + ν_H in a side branch of pp-chain, they would undergo the observable decay into an electron, a positron and a light neutrino νH→νL+e++e−ν_{H}\rightarrowν_{L}+e^++e^-. In the present work Borexino data are used to set a bound on the existence of such decays. We constrain the mixing of a heavy neutrino with mass 1.5 MeV ≤mνH≤\leq m_{ν_{H}} \le 14 MeV to be ∣UeH∣2≤(10−3−4×10−6)|U_{eH}|^2\leq (10^{-3}-4\times10^{-6}) respectively. These are tighter limits on the mixing parameters than obtained in previous experiments at nuclear reactors and accelerators.

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