Definitive measurements of the smallest neutrino mixing angle θ13 were made by Daya Bay, Double Chooz and RENO in 2012, based on the disappearance of electron antineutrinos emitted from reactors. The new generation reactor experiments have significantly improved a sensitivity for θ13 down to the sin2(2θ13)~0.01 level using two identical detectors of 10 ~ 40 tons at near (300 ~ 400 m) and far (1 ~ 2 km) locations. The θ13 measurements by the three reactor experiments are presented with their future expected sensitivities
This article reports an improved independent measurement of neutrino mixing angle θ13 at the Daya Ba...
Angle θ13 is one of the two unknown neutrino mixing parameters to be determined. Its value may deter...
The Reactor Experiment for Neutrino Oscillation (RENO) has been taking data from August, 2011 using ...
Abstract. Definitive measurements of the smallest neutrino mixing angle θ13 were made by Daya Bay, D...
We report an improved measurement of the neutrino mixing angle θ13 from the Daya Bay Reactor Neutrin...
Taking into account recent theoretical and experimental inputs on reactor fluxes we reconsider the d...
With 2.5× the previously reported exposure, the Daya Bay experiment has improved the measurement of ...
AbstractRENO (Reactor Experiment for Neutrino Oscillation) made a definitive measurement of the smal...
Neutrino oscillation with three active neutrinos has been well established by experiments. However, ...
AbstractTaking into account recent theoretical and experimental inputs on reactor fluxes we reconsid...
The Daya Bay reactor neutrino experiment aimed to precisely measure the least known mixing angle θ13...
This document describes the design of the Daya Bay reactor neutrino experiment. Recent discoveries i...
The Daya Bay Reactor Neutrino Experiment was designed to achieve a sensitivity on the value of sin22...
The Daya Bay Reactor Neutrino Experiment was designed to achieve a sensitivity on the value of sin^2...
A measurement of the smallest neutrino mixing angle, $\theta_{13}$, by observations of reactor $\bar...
This article reports an improved independent measurement of neutrino mixing angle θ13 at the Daya Ba...
Angle θ13 is one of the two unknown neutrino mixing parameters to be determined. Its value may deter...
The Reactor Experiment for Neutrino Oscillation (RENO) has been taking data from August, 2011 using ...
Abstract. Definitive measurements of the smallest neutrino mixing angle θ13 were made by Daya Bay, D...
We report an improved measurement of the neutrino mixing angle θ13 from the Daya Bay Reactor Neutrin...
Taking into account recent theoretical and experimental inputs on reactor fluxes we reconsider the d...
With 2.5× the previously reported exposure, the Daya Bay experiment has improved the measurement of ...
AbstractRENO (Reactor Experiment for Neutrino Oscillation) made a definitive measurement of the smal...
Neutrino oscillation with three active neutrinos has been well established by experiments. However, ...
AbstractTaking into account recent theoretical and experimental inputs on reactor fluxes we reconsid...
The Daya Bay reactor neutrino experiment aimed to precisely measure the least known mixing angle θ13...
This document describes the design of the Daya Bay reactor neutrino experiment. Recent discoveries i...
The Daya Bay Reactor Neutrino Experiment was designed to achieve a sensitivity on the value of sin22...
The Daya Bay Reactor Neutrino Experiment was designed to achieve a sensitivity on the value of sin^2...
A measurement of the smallest neutrino mixing angle, $\theta_{13}$, by observations of reactor $\bar...
This article reports an improved independent measurement of neutrino mixing angle θ13 at the Daya Ba...
Angle θ13 is one of the two unknown neutrino mixing parameters to be determined. Its value may deter...
The Reactor Experiment for Neutrino Oscillation (RENO) has been taking data from August, 2011 using ...