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首页> 外文期刊>Nuclear instruments and methods in physics research >Performance of the gamma-ray camera based on GSO(Ce) scintillator array and PSPMT with the ASIC readout system
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Performance of the gamma-ray camera based on GSO(Ce) scintillator array and PSPMT with the ASIC readout system

机译:基于GSO(Ce)闪烁体阵列和带有ASIC读出系统的PSPMT的伽马射线照相机的性能

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We have studied the performance of a readout system with ASIC chips for a gamma-ray camera based on a 64-channel multi-anode PSPMT (Hamamatsu flat-panel H8500) coupled to a GSO(Ce) scintillator array. The GSO array consists of 8 x 8 pixels of 6 × 6 × 13 mm~3 with the same pixel pitch as the anode of the H8500. This camera is intended to serve as an absorber of an electron tracking Compton gamma-ray camera that measures gamma rays up to ~1 MeV. Because we need a readout system with low power consumption for a balloon-borne experiment, we adopted a 32-channel ASIC chip, IDEAS VA32_HDR11,which has one of the widest dynamic range among commercial chips. However, in the case of using a GSO(Ce) crystal and the H8500, the dynamic range of VA32_HDR11 is narrow, and therefore the H8500 has to be operated with a low gain of about 10~5. If the H8500 is operated with a low gain, the camera has a narrow incident-energy dynamic range from 100 to 700keV, and a bad energy resolution of 13.0% (FWHM) at 662 keV. We have therefore developed an attenuator board in order to operate the H8500 with the typical gain of 10~6, which can measure up to ~1 MeV gamma ray. The board makes the variation of the anode gain uniform and widens the dynamic range of the H8500. The system using the new attenuator board has a good uniformity of min:max~1:1.6, an incident-energy dynamic range from 30 to 900 keV, a position resolution of less than 6 mm, and a typical energy resolution of 10.6% (FWHM) at 662 keV with a low power consumption of about 1.7W/64ch.
机译:我们已经研究了基于ASIC芯片的读出系统的性能,该系统基于耦合到GSO(Ce)闪烁体阵列的64通道多阳极PSPMT(滨松H8500平板)的伽马射线照相机。 GSO阵列由6×6×13 mm〜3的8 x 8像素组成,像素间距与H8500的阳极相同。该照相机旨在用作电子跟踪康普顿伽马射线照相机的吸收器,该照相机可测量高达〜1 MeV的伽马射线。由于我们需要一个低功耗的读出系统来进行气球实验,因此我们采用了32通道ASIC芯片IDEAS VA32_HDR11,该芯片是商用芯片中动态范围最广的芯片之一。但是,在使用GSO(Ce)晶体和H8500的情况下,VA32_HDR11的动态范围很窄,因此H8500必须以大约10〜5的低增益工作。如果H8500以低增益运行,则摄像机的入射能量动态范围在100至700keV范围内,在662keV时的能量分辨率为13.0%(FWHM)。因此,我们开发了一种衰减器板,以使H8500能够以10〜6的典型增益工作,它可以测量高达〜1 MeV的伽马射线。该板使阳极增益的变化均匀,并扩大了H8500的动态范围。使用新型衰减器板的系统具有极好的min:max〜1:1.6均匀性,入射能量动态范围为30到900 keV,位置分辨率小于6 mm,典型能量分辨率为10.6%( FWHM)在662 keV时具有约1.7W / 64ch的低功耗。

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