From f8698c968f852b99590008190f7d3738be36e0b6 Mon Sep 17 00:00:00 2001 From: patricksecrest Date: Sun, 28 Sep 2025 00:15:37 +0800 Subject: [PATCH] Add 'Satellite GPS Tracker' --- Satellite-GPS-Tracker.md | 9 +++++++++ 1 file changed, 9 insertions(+) create mode 100644 Satellite-GPS-Tracker.md diff --git a/Satellite-GPS-Tracker.md b/Satellite-GPS-Tracker.md new file mode 100644 index 0000000..7cc4242 --- /dev/null +++ b/Satellite-GPS-Tracker.md @@ -0,0 +1,9 @@ +
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The results obtained in laboratory checks, using scintillator bars learn by silicon photomultipliers are reported. The current approach is the first step for designing a precision tracking system to be placed inside a free magnetized volume for the charge identification of low energy crossing particles. The devised system is demonstrated in a position to offer a spatial decision higher than 2 mm. Scintillators, Photon Solid State detector, [iTagPro device](https://imoodle.win/wiki/6_Best_Free_Phone_Tracker_Apps_Android_-_IPhone_In_2025) particle monitoring gadgets. Among the planned activities was the construction of a gentle 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 [iTagPro key finder](https://opensourcebridge.science/wiki/User:TriciaMaccallum) charge 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 volume. In this paper we report the outcomes obtained with a small array of triangular scintillator [ItagPro](https://botdb.win/wiki/ITagPro_Tracker:_The_Ultimate_Bluetooth_Locator_Device) bars coupled to silicon photomultiplier (SiPM) with wavelength shifter (WLS) fibers.
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This bar profile is here demonstrated able to offer the required spatial decision in reconstructing the position of the crossing particle by profiting of the cost-sharing between adjacent bars readout in analog mode. SiPMs are glorious candidates in changing standard photomultipliers in lots of experimental conditions. Tests have been performed with laser beam pulses and radioactive supply in order to characterize the scintillator bar response and SiPM behaviour. Here we briefly current the noticed behaviour of the SiPM used in our assessments relating to the primary sources of noise and the effect of temperature on its response and linearity. Several models and packaging have been thought-about. The main source of noise which limits the SiPM’s single photon decision is the "dark current" charge. It is originated by cost carriers thermally created within the delicate quantity and [iTagPro device](https://nerdgaming.science/wiki/User:ValerieMajeski) current within the conduction band and subsequently it depends upon the temperature. The dependence of the darkish current single pixel rate as a function of the temperature has been investigated utilizing Peltier cells in order to change and keep the temperature managed.
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Dark present fee relies upon additionally on the Vwk as proven in Fig. 3. As a way to have low rates of dark present the value of Vbias has been fastened at 1.5 V giving a working voltage Vwk of 29 V. It is clear that, if necessary, it may be handy to use a bias voltage regulator [itagpro device](https://timeoftheworld.date/wiki/Avoid_Missed_Renewals_With_Automated_Registration_And_Certification_Tracking) which mechanically compensates for temperature variations. Not all the time the pixels of the SiPM work independently from each other. Photoelectrons (p.e.) can migrate from the hit pixel to a different 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 chance might be obtained by the ratio double-to-single pulse price as a perform of the temperature. The probability relies upon weakly on the temperature and the measured stage of cross-speak (15-16%) is compatible with the one reported in the datasheet. SiPM response as soon as its primary parameters and cells configuration are given.
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