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The outcomes obtained in laboratory tests, utilizing scintillator bars learn by silicon photomultipliers are reported. The current approach is the first step for designing a precision monitoring system to be placed inside a free magnetized quantity for the charge identification of low vitality crossing particles. The devised system is demonstrated able to provide a spatial resolution better than 2 mm. Scintillators, ItagPro Photon Solid State detector, particle monitoring units. Among the many deliberate actions was the construction of a light spectrometer seated in a 20-30 m3 magnetized air volume, the Air Core Magnet (ACM). The whole design needs to be optimised for iTagPro geofencing the willpower of the momentum and cost of muons within the 0.5 - 5 GeV/c range (the mis-identification is required to be lower than 3% at 0.5 GeV/c). 1.5 mm is required contained in the magnetized air quantity. On this paper we report the results obtained with a small array of triangular scintillator iTagPro website bars coupled to silicon photomultiplier (SiPM) with wavelength shifter (WLS) fibers.
This bar profile is here demonstrated ready to offer the mandatory spatial resolution in reconstructing the position of the crossing particle by profiting of the charge-sharing between adjoining bars readout in analog mode. SiPMs are wonderful candidates in changing customary photomultipliers in many experimental conditions. Tests have been carried out with laser beam pulses and radioactive source with a purpose to characterize the scintillator bar response and SiPM behaviour. Here we briefly current the observed behaviour of the SiPM utilized in our checks regarding the main sources of noise and iTagPro website the impact of temperature on its response and linearity. Several models and iTagPro website packaging have been considered. The primary source of noise which limits the SiPM’s single photon decision is the "dark current" rate. It is originated by cost carriers thermally created within the delicate quantity and current in the conduction band and therefore it relies on the temperature. The dependence of the dark present single pixel charge as a operate of the temperature has been investigated using Peltier cells in order to vary and keep the temperature managed.
Dark current charge depends also on the Vwk as proven in Fig. 3. In an effort to have low rates of dark current the value of Vbias has been mounted at 1.5 V giving a working voltage Vwk of 29 V. It is obvious that, if needed, it may be convenient to make use of a bias voltage regulator which automatically compensates for temperature variations. Not all the time the pixels of the SiPM work independently from one another. Photoelectrons (p.e.) can migrate from the hit pixel to another not directly fired by a photon. Optical cross-talk between pixels leads to a non-Poissonian behaviour of the distribution of fired pixels. An estimate of the optical cross speak probability may be obtained by the ratio double-to-single pulse charge as a operate of the temperature. The likelihood depends weakly on the temperature and the measured degree of cross-talk (15-16%) is suitable with the one reported in the datasheet. SiPM response as soon as its basic parameters and cells configuration are given.