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The entire design needs to be optimised for the determination of the momentum and cost 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 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.&lt;br&gt; &lt;br&gt;&lt;br&gt;&lt;br&gt;This bar profile is here demonstrated ready to offer the mandatory spatial resolution in reconstructing the place 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 lots of experimental conditions. Tests have been carried out with laser beam pulses and radioactive source in an effort to characterize the scintillator bar response and SiPM behaviour. Here we briefly current the noticed behaviour of the SiPM utilized in our tests regarding the principle sources of noise and the impact of temperature on its response and linearity. Several fashions and packaging have been thought-about. The principle supply of noise which limits the SiPM’s single photon decision is the &quot;dark current&quot; price. It&#039;s originated by cost carriers thermally created within the sensitive quantity and present within the conduction band and therefore it depends on the temperature. The dependence of the dark current single pixel price as a function of the temperature has been investigated utilizing Peltier cells so as to change and keep the temperature controlled.&lt;br&gt;&lt;br&gt;&lt;br&gt;&lt;br&gt;Dark current fee relies upon also on the Vwk as shown in Fig. 3. So as to have low rates of darkish current the worth of Vbias has been fastened at 1.5 V giving a working voltage Vwk of 29 V. It is obvious that, if necessary, it can be handy to use a bias voltage regulator which mechanically compensates for temperature variations. Not at all times the pixels of the SiPM work independently from one another. Photoelectrons (p.e.) can migrate from the hit pixel to another 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 discuss likelihood might be obtained by the ratio double-to-single pulse charge as a perform of the temperature. The likelihood relies upon weakly on the temperature and the measured degree of cross-talk (15-16%) is compatible with the one reported in the datasheet. SiPM response once its primary parameters and cells configuration are given.&lt;br&gt;&lt;br&gt;&lt;br&gt;&lt;br&gt;Within the Fig. 4 it&#039;s proven the pulse peak distribution of the dark current for the SiPM under test. 0.2) mm diameter gap used to lodge a fiber to gather the sunshine. The lateral floor of the scintillator strips is painted with white EJ-510 TiO2 Eljen paint. The scintillation mild is collected with 1.2 mm BCF-91A WaveLength Shifter (WLS) fiber produced by the Saint-Gobain Ltd. The WLS is glued into the opening operating along the bar and its ends are polished. The read-out is carried out by the SiPM solely at one finish and the opposite facet is mirrored with reflecting tape to maximize the sunshine collection. The entrance-end board prototype devoted to the amplification and SiPM readout has been developed by the Bologna INFN electronic group. 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