Leading Fleet Tracking Solutions
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The outcomes obtained in laboratory exams, utilizing scintillator bars read by silicon photomultipliers are reported. The current method is step one for designing a precision tracking system to be positioned inside a free magnetized quantity for iTagPro smart tracker the cost identification of low vitality crossing particles. The devised system is demonstrated able to offer 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 gentle spectrometer seated in a 20-30 m3 magnetized air quantity, bluetooth keychain tracker the Air Core Magnet (ACM). The whole design needs to be optimised for the determination of the momentum and iTagPro 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 inside the magnetized air quantity. 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 right here demonstrated in a position to provide the necessary spatial decision in reconstructing the position of the crossing particle by profiting of the charge-sharing between adjacent bars readout in analog mode. SiPMs are wonderful candidates in changing normal photomultipliers in many experimental circumstances. Tests have been carried out with laser beam pulses and radioactive source with a purpose to characterize the scintillator bar response and iTagPro shop SiPM behaviour. Here we briefly present the observed behaviour of the SiPM used in our exams relating to the primary sources of noise and the impact of temperature on its response and linearity. Several fashions and packaging have been thought of. The primary supply of noise which limits the SiPM’s single photon decision is the "dark current" fee. It's originated by charge carriers thermally created in the delicate volume and ItagPro present within the conduction band and subsequently it will depend on the temperature. The dependence of the dark current single pixel rate as a perform of the temperature has been investigated using Peltier cells so as to change and keep the temperature controlled.
Dark current charge depends also on the Vwk as shown in Fig. 3. With a purpose to have low rates of darkish present the value of Vbias has been fixed at 1.5 V giving a working voltage Vwk of 29 V. It is evident that, if necessary, it may be convenient to make use of a bias voltage regulator which automatically compensates for ItagPro temperature variations. Not always the pixels of the SiPM work independently from one another. Photoelectrons (p.e.) can migrate from the hit pixel to a different indirectly 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 probability will be obtained by the ratio double-to-single pulse rate as a function of the temperature. The chance depends weakly on the temperature and ItagPro the measured level of cross-talk (15-16%) is compatible with the one reported in the datasheet. SiPM response once its basic parameters and cells configuration are given.