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The results obtained in laboratory checks, utilizing scintillator bars read by silicon photomultipliers are reported. The present method is step one for designing a precision tracking system to be placed inside a free magnetized volume for ItagPro the charge identification of low power crossing particles. The devised system is demonstrated ready to provide a spatial decision better than 2 mm. Scintillators, Photon Solid State detector, particle tracking units. Among the many deliberate activities was the development of a light spectrometer seated in a 20-30 m3 magnetized air quantity, the Air Core Magnet (ACM). The whole design should be optimised for the determination of the momentum and charge of muons in the 0.5 - 5 GeV/c range (the mis-identification is required to be less 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 bars coupled to silicon photomultiplier (SiPM) with wavelength shifter (WLS) fibers.
This bar profile is here demonstrated able to provide the necessary spatial decision in reconstructing the place of the crossing particle by profiting of the cost-sharing between adjoining bars readout in analog mode. SiPMs are glorious candidates in changing commonplace photomultipliers in many experimental situations. Tests have been performed with laser beam pulses and ItagPro radioactive source in order to characterize the scintillator bar response and SiPM behaviour. Here we briefly present the observed behaviour of the SiPM used in our assessments regarding the principle sources of noise and the impact of temperature on its response and linearity. Several models and packaging have been thought-about. The main source of noise which limits the SiPM’s single photon decision is the "dark current" price. It's originated by charge carriers thermally created in the sensitive volume and ItagPro present within the conduction band and ItagPro due to this fact it is dependent upon the temperature. The dependence of the darkish present single pixel charge as a function of the temperature has been investigated using Peltier cells in order to change and keep the temperature controlled.
Dark current charge relies upon also on the Vwk as proven in Fig. 3. In an effort to have low rates of dark present the value of Vbias has been fastened at 1.5 V giving a working voltage Vwk of 29 V. It is evident that, ItagPro if crucial, it can be convenient to use a bias voltage regulator which robotically compensates for temperature variations. Not at all times the pixels of the SiPM work independently from each other. Photoelectrons (p.e.) can migrate from the hit pixel to a different in a roundabout way fired by a photon. Optical cross-speak between pixels leads to a non-Poissonian behaviour of the distribution of fired pixels. An estimate of the optical cross discuss probability might be obtained by the ratio double-to-single pulse price as a function of the temperature. The probability relies upon weakly on the temperature and the measured level of cross-talk (15-16%) is suitable with the one reported within the datasheet. SiPM response once its primary parameters and cells configuration are given.