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The outcomes obtained in laboratory exams, using scintillator bars learn 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 the charge identification of low vitality crossing particles. The devised system is demonstrated able to provide a spatial decision better than 2 mm. Scintillators, Photon Solid State detector, particle tracking devices. Among the planned actions was the construction of a mild spectrometer seated in a 20-30 m3 magnetized air quantity, the Air Core Magnet (ACM). The whole design needs to be optimised for the determination of the momentum and cost of muons in the 0.5 - 5 GeV/c vary (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 volume. In this paper we report the outcomes 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 ready to provide the mandatory spatial decision in reconstructing the position of the crossing particle by profiting of the cost-sharing between adjoining bars readout in analog mode. SiPMs are excellent candidates in changing commonplace photomultipliers in many experimental circumstances. Tests have been carried out with laser beam pulses and iTagPro reviews radioactive source with a view to characterize the scintillator bar response and iTagPro SiPM behaviour. Here we briefly present the noticed behaviour of the SiPM used in our tests regarding the principle sources of noise and the effect of temperature on its response and linearity. Several fashions and packaging have been considered. The main supply of noise which limits the SiPM’s single photon resolution is the "dark current" rate. It's originated by cost carriers thermally created within the sensitive volume and present within the conduction band and due to this fact it will depend on the temperature. The dependence of the dark present single pixel price as a function of the temperature has been investigated utilizing Peltier cells so as to change and keep the temperature managed.



Dark current fee depends also on the Vwk as proven in Fig. 3. With a view to have low charges of darkish current the worth of Vbias has been fixed at 1.5 V giving a working voltage Vwk of 29 V. It is obvious that, iTagPro reviews if essential, it can be handy to make use of a bias voltage regulator which automatically compensates for temperature variations. Not always the pixels of the SiPM work independently from one another. Photoelectrons (p.e.) can migrate from the hit pixel to another in a roundabout way fired by a photon. Optical cross-speak between pixels results in a non-Poissonian behaviour of the distribution of fired pixels. An estimate of the optical cross talk chance will be obtained by the ratio double-to-single pulse rate as a operate of the temperature. The probability relies upon weakly on the temperature and the measured level of cross-discuss (15-16%) is suitable with the one reported in the datasheet. SiPM response as soon as its primary parameters and cells configuration are given.



In the Fig. Four it is shown the pulse peak distribution of the dark present for iTagPro reviews the SiPM beneath take a look at. 0.2) mm diameter gap used to lodge a fiber to gather the sunshine. The lateral surface of the scintillator strips is painted with white EJ-510 TiO2 Eljen paint. The scintillation light is collected with 1.2 mm BCF-91A WaveLength Shifter (WLS) fiber produced by the Saint-Gobain Ltd. The WLS is glued into the hole running alongside the bar and its ends are polished. The learn-out is carried out by the SiPM solely at one finish and the alternative facet is mirrored with reflecting tape to maximise the sunshine collection. The front-end board prototype dedicated to the amplification and SiPM readout has been developed by the Bologna INFN digital group. The present from the SiPM is discharged on the low enter resistance of the transimpedance amplifier; this offers small time constants, that is, fast sign rise time (using the OPA 656N with a 500 MHz bandwidth we acquire indicators with 20-30 ns of rise time).