Abstract:Abstract-The response of a silicon photomultiplier (SiPM) to optical signals is inherently nonproportional due to saturation, afterpulsing, and crosstalk. Existing models of the SiPM response do not account for all of these effects, and therefore, these models are not sufficiently accurate for many applications. In this work, a comprehensive model of the SiPM response is developed that is generally applicable to exponentially decaying light pulses and that can be simplified in the case of very short (e.g., las… Show more
“…Hence there is a trade-off between the geometry, the dimensions and number of microcells for a given area, the PDE and the dynamic range. A more complex model of the response of an SiPM sensor that takes into account the effects of the recovery time, afterpulsing and crosstalk has also been developed [32]. Figure 4 shows the photopeak mean height as a function of gamma energy at 2, 3, 4 and 5V above the SiPM breakdown voltage.…”
Abstract-Scintillators are a critical component of sensor systems for the detection of ionizing radiation. Such systems have a diverse portfolio of applications from medical imaging, well logging in oil exploration and detection systems for the prevention of the illicit movement of nuclear materials. The rare earth element cerium is an ideal dopant for a variety of host scintillating materials due to the fast 5d1 → 4f radiative transition of Ce 3+ . Cerium-doped Gadolinium Aluminium Gallium Garnet (Ce:GAGG) is a relatively new single crystal scintillator with several interesting properties. These include high light yield; an emission peak well-matched to silicon sensors; and a low intrinsic energy resolution. Moreover, the material has a high density and is non-hygroscopic. In this article we review the properties of cerium-doped GAGG and report Energy Resolution (ER) measurements over the temperature range -10• C to +50• C for 3 × 3 × 30 mm 3 Ce:GAGG crystals optically coupled to a Silicon Photomultipler (SiPM) sensor with a 3mm × 3mm active area. In addition the linearity of the scintillator-SiPM response as a function of gamma energy is reported.
“…Hence there is a trade-off between the geometry, the dimensions and number of microcells for a given area, the PDE and the dynamic range. A more complex model of the response of an SiPM sensor that takes into account the effects of the recovery time, afterpulsing and crosstalk has also been developed [32]. Figure 4 shows the photopeak mean height as a function of gamma energy at 2, 3, 4 and 5V above the SiPM breakdown voltage.…”
Abstract-Scintillators are a critical component of sensor systems for the detection of ionizing radiation. Such systems have a diverse portfolio of applications from medical imaging, well logging in oil exploration and detection systems for the prevention of the illicit movement of nuclear materials. The rare earth element cerium is an ideal dopant for a variety of host scintillating materials due to the fast 5d1 → 4f radiative transition of Ce 3+ . Cerium-doped Gadolinium Aluminium Gallium Garnet (Ce:GAGG) is a relatively new single crystal scintillator with several interesting properties. These include high light yield; an emission peak well-matched to silicon sensors; and a low intrinsic energy resolution. Moreover, the material has a high density and is non-hygroscopic. In this article we review the properties of cerium-doped GAGG and report Energy Resolution (ER) measurements over the temperature range -10• C to +50• C for 3 × 3 × 30 mm 3 Ce:GAGG crystals optically coupled to a Silicon Photomultipler (SiPM) sensor with a 3mm × 3mm active area. In addition the linearity of the scintillator-SiPM response as a function of gamma energy is reported.
“…However, SiPM performance in photon number and time resolution in the case of short pulse detection is comprehensively modelled due to its high practical importance [11,12], but results have rather limited applicability to Fig. 1.…”
“…4 are presented on a single graph. The easiest way of determining parameters a, b and c is to minimize the weight mean square error between the measured data y i and the LevenbergMarquardt best fit function G(V i ,T i ,a,b,c) (2). N is the number of data points.…”
Section: Gain Stabilization Algorithmmentioning
confidence: 99%
“…two photons fall into arrays of pixels then two avalanches are triggered and the total output signal is twice as high as in the case of one photon. A SiPM is able to detect light on the level of single photons due to high gain (10 6 ) [1,2,3]. The gain of a SiPM is strongly dependent on temperature.…”
The paper stresses the issue of strong temperature influence on the gain of a Silicon Photomultiplier (SiPM). High sensitivity of the detector to light (single photons) requires stable parameters during measurement, including gain. The paper presents a method of compensating the change of gain caused by temperature variations, by adjusting a suitable voltage bias provided by a precise power module. The methodology of the research takes in account applications with a large number of SiPMs (20 thousand), explains the challenges and presents the results of the gain stabilization algorithm.
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