In the Neutrino Physics Field, a lot of careful measurements am made such as : cross section measure¬ment, neutrino oscillation, atmospheric neutrino. Etc. In such experimental measurements one has to get the most accurate numbers as possible but in doing so one meets a lot of constraints and variables. Such is the case of the Test Beam detector (a replica of the full MIN HR//A detector where we lest and compare new targets and devices to put them further in the MINERr/A detector). The way we detect some signal in the detector is by using a scintillator material attached to a photomultiplier (when a charged particle passes through the scintillator, this emits a photon of certain spectra and this light works as input for the PMT which uses the photoelectric effect to magnify the signal (gain)), in the same way the PMT is wired to the Data Acquisition System (DAQ) in order to process the ...

In the Neutrino Physics Field, a lot of careful measurements am made such as : cross section measure¬ment, neutrino oscillation, atmospheric neutrino. Etc. In such experimental measurements one has to get the most accurate numbers as possible but in doing so one meets a lot of constraints and variables. Such is the case of the Test Beam detector (a replica of the full MIN HR//A detector where we lest and compare new targets and devices to put them further in the MINERr/A detector). The way we detect some signal in the detector is by using a scintillator material attached to a photomultiplier (when a charged particle passes through the scintillator, this emits a photon of certain spectra and this light works as input for the PMT which uses the photoelectric effect to magnify the signal (gain)), in the same way the PMT is wired to the Data Acquisition System (DAQ) in order to process the ...