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(Image: https://picography.co/wp-content/uploads/2019/10/picography-casual-mens-fashion-in-india-600x400.jpg)The results obtained in laboratory tests, utilizing scintillator bars learn by silicon photomultipliers are reported. The present method is step one for iTagPro support designing a precision monitoring system to be placed inside a free magnetized quantity for the cost identification of low power crossing particles. The devised system is demonstrated able to offer a spatial resolution better than 2 mm. Scintillators, Photon Solid State detector, particle monitoring units. Among the many planned activities was the development 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 dedication of the momentum and charge of muons in the 0.5 - 5 GeV/c vary (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. In 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 right here demonstrated able to offer the required spatial decision in reconstructing the place of the crossing particle by profiting of the cost-sharing between adjacent bars readout in analog mode. SiPMs are wonderful candidates in replacing normal photomultipliers in many experimental circumstances. Tests have been performed with laser beam pulses and iTagPro support radioactive supply with a purpose to characterize the scintillator bar response and SiPM behaviour. Here we briefly present the noticed behaviour of the SiPM utilized in our exams regarding the main sources of noise and the effect of temperature on its response and linearity. Several models and packaging have been considered. The primary supply of noise which limits the SiPM’s single photon decision is the “dark current” fee. It is originated by charge carriers thermally created in the sensitive volume and ItagPro present in the conduction band and due to this fact it depends on the temperature. The dependence of the dark present single pixel charge as a function of the temperature has been investigated using Peltier cells so as to change and keep the temperature managed.
Dark current fee relies upon additionally on the Vwk as shown in Fig. 3. So as to have low rates of darkish present the value of Vbias has been fastened at 1.5 V giving a working voltage Vwk of 29 V. It is obvious that, if needed, it can be convenient to use a bias voltage regulator which mechanically compensates for temperature variations. Not always the pixels of the SiPM work independently from each other. 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 speak likelihood will be obtained by the ratio double-to-single pulse fee as a perform of the temperature. The chance 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 as soon as its basic parameters and cells configuration are given.