GPS Tracking Blog

Our latest launch, ItagPro the World Tracker OBD GPS gadget for car tracking is designed to plug in to the OBD diagnostic port of any car, ItagPro providing a fast and dependable choice in GPS tracking methods.Easily installed in minutes, the tracking device requires a knowledge SIM card for operation, and is outfitted with a motion detection sensor to conserve power when the automobile will not be transferring. The GPS tracking device features G-power monitoring for harsh driving detection, real time GPS monitoring, iTagPro technology GPRS communication modes by UDP or TCP, longitude and latitude location, GSM cellular management, and compatibility with any GSM carrier. The device affords a scorching start time of lower than one second. The WT-OBD is compatible with any GPS monitoring software program, including TrackingTheWorld software program which permits customers to monitor the tracker’s location, iTagPro technology set digital boundaries generally known as geo-fences, and create custom-made studies. TrackingTheWorld GPS tracking software also helps JPG and shapefiles. Read extra concerning the WorldTracker OBD. Want extra GPS tracking information and iTagPro technology special gives? Join our electronic mail record!



The results obtained in laboratory tests, using scintillator bars read by silicon photomultipliers are reported. The current method is step one for iTagPro technology designing a precision tracking system to be placed inside a free magnetized quantity for the charge identification of low vitality crossing particles. The devised system is demonstrated in a position to provide a spatial decision better than 2 mm. Scintillators, iTagPro technology Photon Solid State detector, particle tracking devices. Among the planned actions was the construction of a gentle spectrometer seated in a 20-30 m3 magnetized air quantity, the Air Core Magnet (ACM). The entire design should be optimised for the dedication of the momentum and cost of muons in 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 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 in a position to provide the necessary spatial decision in reconstructing the place of the crossing particle by profiting of the charge-sharing between adjoining bars readout in analog mode. SiPMs are excellent candidates in changing normal photomultipliers in many experimental conditions. Tests have been performed with laser beam pulses and radioactive source so as to characterize the scintillator bar response and SiPM behaviour. Here we briefly current the observed behaviour of the SiPM utilized in our exams relating to the principle sources of noise and the impact of temperature on its response and linearity. Several fashions and iTagPro technology packaging have been thought-about. The main supply of noise which limits the SiPM’s single photon resolution is the "dark current" price. It is originated by cost carriers thermally created in the sensitive quantity and present within the conduction band and subsequently it will depend on the temperature. The dependence of the dark present single pixel rate as a function of the temperature has been investigated using Peltier cells in order to vary and keep the temperature controlled.



Dark present price relies upon additionally on the Vwk as proven in Fig. 3. With a purpose to have low rates of dark present the value of Vbias has been mounted at 1.5 V giving a working voltage Vwk of 29 V. It is obvious that, if crucial, it can be convenient to use a bias voltage regulator which automatically 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 not directly fired by a photon. Optical cross-discuss between pixels results in a non-Poissonian behaviour of the distribution of fired pixels. An estimate of the optical cross speak chance may be obtained by the ratio double-to-single pulse charge as a perform of the temperature. The probability relies upon weakly on the temperature and the measured level of cross-talk (15-16%) is appropriate with the one reported in the datasheet. SiPM response once its primary parameters and cells configuration are given.