The Double Chooz experiment measures the neutrino mixing angle θ13 by detecting reactor ¯νe via inverse beta decay. The positron-neutron space and time coincidence allows for a sizable background rejection, nonetheless liquid scintillator detectors would profit from a positron/electron discrimination, if feasible in large detector, to suppress the remaining background. Standard particle identification, based on particle dependent time profile of photon emission in liquid scintillator, can not be used given the identical mass of the two particles. However, the positron annihilation is sometimes delayed by the orthopositronium (o-Ps) metastable state formation, which induces a pulse shape distortion that could be used for positron identificat...
International audiencePulse shape discrimination is a well-established technique for background reje...
We describe a system designed to re-bunch positron pulses delivered by an accumulator supplied by a ...
The Double Chooz collaboration presents a measurement of the neutrino mixing angle θ13 using reactor...
The Double Chooz experiment measures the neutrino mixing angle $\theta_{13}$ by detecting reactor $\...
The Double Chooz experiment measures the neutrino mixing angle θ13 by detecting reactor ν¯e via inve...
International audienceThe aim of the Double Chooz experiment is to measure the neutrino mixing angle...
AbstractThe aim of the Double Chooz experiment is to measure the neutrino mixing angle θ13 by detect...
This article describes the setup and performance of the near and far detectors in the Double Chooz e...
The measurement of the theta-13 mixing angle, to which the Double Chooz experiment contributed, pave...
AbstractWe describe a system designed to re-bunch positron pulses delivered by an accumulator suppli...
International audiencePulse shape discrimination is a well-established technique for background reje...
We describe a system designed to re-bunch positron pulses delivered by an accumulator supplied by a ...
The Double Chooz collaboration presents a measurement of the neutrino mixing angle θ13 using reactor...
The Double Chooz experiment measures the neutrino mixing angle $\theta_{13}$ by detecting reactor $\...
The Double Chooz experiment measures the neutrino mixing angle θ13 by detecting reactor ν¯e via inve...
International audienceThe aim of the Double Chooz experiment is to measure the neutrino mixing angle...
AbstractThe aim of the Double Chooz experiment is to measure the neutrino mixing angle θ13 by detect...
This article describes the setup and performance of the near and far detectors in the Double Chooz e...
The measurement of the theta-13 mixing angle, to which the Double Chooz experiment contributed, pave...
AbstractWe describe a system designed to re-bunch positron pulses delivered by an accumulator suppli...
International audiencePulse shape discrimination is a well-established technique for background reje...
We describe a system designed to re-bunch positron pulses delivered by an accumulator supplied by a ...
The Double Chooz collaboration presents a measurement of the neutrino mixing angle θ13 using reactor...