Abstract <p>The Daya Bay reactor antineutrino experiment was designed to precisely measure the smallest neutrino mixing angle <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\theta_{13}\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m1--> </InlineEquation>. It has collected <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(5.55\times 10^{6}\bar{\nu}_{e}\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m2--> </InlineEquation> events on distances from 360 to 1900 m between reactors and detectors. Detailed analysis of full data set, 3158 days of operation, gives the world-leading measurement of <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\theta_{13}\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m3--> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\sin^{2}2\theta_{13}=0.0851\pm 0.0024\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m4--> </InlineEquation>. The mass splitting is <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\Delta m_{32}^{2}=(2.466\pm 0.060)\times 10^{{-}3}\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m5--> </InlineEquation> eV<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({}^{2}\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m6--> </InlineEquation> assuming the normal mass ordering or <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\Delta m_{32}^{2}={-}(2.571\pm 0.060)\times 10^{{-}3}\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m7--> </InlineEquation> eV<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\({}^{2}\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m8--> </InlineEquation> assuming the inverted mass ordering. The results of the search for sterile neutrino show no significant signal. Obtained with CL<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\({}_{s}\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m9--> </InlineEquation> method result provides the world’s stringent exclusion of the sterile amplitude <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\sin^{2}2\theta_{14}\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m10--> </InlineEquation> in a wide range of sterile mass splittings: <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(2\times 10^{{-}4}\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m11--> </InlineEquation> eV<InlineEquation ID="IEq12"> <EquationSource Format="TEX">\({}^{2}\lesssim\Delta m_{41}^{2}\lesssim 0.3\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m12--> </InlineEquation> eV<InlineEquation ID="IEq13"> <EquationSource Format="TEX">\({}^{2}\)</EquationSource> <!--NuclPhys2560165Zavadskyi-m13--> </InlineEquation>.</p>

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The Latest Results of the Daya Bay Reactor Antineutrino Experiment

  • V. Zavadskyi

摘要

Abstract

The Daya Bay reactor antineutrino experiment was designed to precisely measure the smallest neutrino mixing angle \(\theta_{13}\) . It has collected \(5.55\times 10^{6}\bar{\nu}_{e}\) events on distances from 360 to 1900 m between reactors and detectors. Detailed analysis of full data set, 3158 days of operation, gives the world-leading measurement of \(\theta_{13}\) , \(\sin^{2}2\theta_{13}=0.0851\pm 0.0024\) . The mass splitting is \(\Delta m_{32}^{2}=(2.466\pm 0.060)\times 10^{{-}3}\) eV \({}^{2}\) assuming the normal mass ordering or \(\Delta m_{32}^{2}={-}(2.571\pm 0.060)\times 10^{{-}3}\) eV \({}^{2}\) assuming the inverted mass ordering. The results of the search for sterile neutrino show no significant signal. Obtained with CL \({}_{s}\) method result provides the world’s stringent exclusion of the sterile amplitude \(\sin^{2}2\theta_{14}\) in a wide range of sterile mass splittings: \(2\times 10^{{-}4}\) eV \({}^{2}\lesssim\Delta m_{41}^{2}\lesssim 0.3\) eV \({}^{2}\) .