Locate high-worth assets the second you want them. No more concern of asset theft. Why Choose BLE Asset Tracking Tag? How Does BLE Asset Tracking Tag Work? A Bluetooth Asset Tracking Tag is a small, wireless Bluetooth beacon that may be hooked up to belongings similar to equipment, iTagPro machinery, or ItagPro tools. It uses Bluetooth gateway to speak with close by smartphones or tablets working a suitable app. The app allows users to trace the situation of the property and monitor their movement in real-time. Why select MOKOSMART BLE Asset Tracking Tag? MOKOSMART is a leading manufacturers of asset tracking ODMs and OEMs. Over 1 million devices have been deployed in more than 120 international locations. Along with Bluetooth connectivity, we also have Wif, ItagPro RFID, Cellular (2G, 3G, LTE-M/NB-IoT) and ItagPro LoRaWAN options. Our commitment to top quality experience in low energy design means our devices carry out better and final longer than our rivals. Our aseet tracking tag protects your data with AES-128 (LoRaWAN) and AES-256 (cellular) encryption. With custom firmware and iTagPro online sensor integration, we modify the current devices range to suit area of interest functions, saving you money and time. As a renowned loT units solution provider, MOKO Smart can ensure that your mission is main the industry. Choose us to provide you with OEM or ODM services.
The results obtained in laboratory tests, ItagPro utilizing scintillator bars read by silicon photomultipliers are reported. The present strategy is step one for designing a precision monitoring system to be placed inside a free magnetized volume for the charge identification of low power crossing particles. The devised system is demonstrated able to supply a spatial decision higher than 2 mm. Scintillators, ItagPro Photon Solid State detector, ItagPro particle monitoring gadgets. Among the many planned actions was the development of a light spectrometer seated in a 20-30 m3 magnetized air volume, ItagPro the Air Core Magnet (ACM). The entire design ought to be optimised for the determination of the momentum and charge 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 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 here demonstrated ready to supply the mandatory 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 glorious candidates in replacing customary photomultipliers in many experimental conditions. Tests have been performed with laser beam pulses and radioactive source as a way to characterize the scintillator bar response and SiPM behaviour. Here we briefly current the observed behaviour of the SiPM used in our tests regarding the main sources of noise and the effect of temperature on its response and ItagPro linearity. Several models and packaging have been considered. The principle supply of noise which limits the SiPM’s single photon resolution is the "dark current" price. It's originated by charge carriers thermally created in the sensitive quantity and present in the conduction band and due to this fact it is determined by the temperature. The dependence of the darkish current single pixel fee as a function of the temperature has been investigated using Peltier cells so as to alter and keep the temperature managed.
Dark current price relies upon additionally on the Vwk as proven in Fig. 3. With a purpose 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 if crucial, it can be convenient to make use of a bias voltage regulator which robotically 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 another not directly fired by a photon. Optical cross-talk between pixels results in a non-Poissonian behaviour of the distribution of fired pixels. An estimate of the optical cross talk likelihood might be obtained by the ratio double-to-single pulse charge as a operate of the temperature. The likelihood depends weakly on the temperature and the measured stage of cross-discuss (15-16%) is suitable with the one reported in the datasheet. SiPM response once its basic parameters and cells configuration are given.