SiPM-GAGG(Ce)探测器γ能谱稳谱方法研究

Study on Gamma Spectrum Stabilization Method for SiPM-GAGG(Ce) Detector

  • 摘要: 硅光电倍增管(silicon photomultiplier, SiPM)作为21世纪以来新型光电转换器件,具有高增益、低功耗等优点,广泛应用于医疗成像、高能物理、环境监测以及国防安全等领域。硅光电倍增管耦合铈掺杂钆镓铝石榴石(GAGG(Ce))晶体组成的探测器在能谱测量及成像探测中具有广泛应用前景。本文研究了一款8×8阵列型SiPM耦合Φ2 in×2 in GAGG(Ce)晶体探测器的温度漂移特性,设计搭建了一套基于温度传感器反馈调节SiPM-GAGG(Ce)探测器工作电压的增益补偿系统。分别进行了电源可靠性测试、电源纹波测试以及温度补偿测试等实验。实验结果表明,电源长期工作稳定性高,电源纹波系数小于0.001%。在-20~40 ℃的温度范围内,实测137Cs、60Co、241Am放射源γ能谱的662、1 173、1 332、59.5 keV全能峰最大峰位道址为515.9、915.8、1 041.0、43.1道,最小峰位道址为507.1、899.0、1 022.9、43.1道,最大正向漂移分别为4.6、7.8、8.3、0.5道,最大负向漂移分别为4.2、8.7、9.8、0.5道。137Cs全能峰峰位道址平均漂移率从45.34%降到0.37%,137Cs能量分辨率从-20 ℃的8.36%变化到40 ℃时的9.29%,显著提高了γ能谱测量系统的稳定性。

     

    Abstract: Silicon photomultiplier (SiPM) is a new type of photoelectric conversion device with high gain and low power consumption since the 21st century. It consists of thousands of single photon avalanche diodes (SPADs) operating in Geiger mode connected in parallel with each other. It is widely used in medical imaging, high-energy physics, environmental monitoring and defence and security. The SiPM coupled with cerium-doped gadolinium gallium aluminium garnet (GAGG(Ce)) crystals is a promising detector for energy spectrum measurement and imaging detection. In this paper, the temperature drift characteristics of an 8×8 array SiPM-coupled Φ2 in×2 in GAGG(Ce) crystal detector were investigated, and a gain compensation system based on the feedback adjustment of the operating voltage of the SiPM-GAGG(Ce) detector by a temperature sensor was designed and built. Experiments such as power supply reliability test, power supply ripple test and temperature compensation test were carried out separately. The experimental results show that the power supply has high long-term operating stability and the power supply ripple noise is less than 0.001%. The output voltage range is 0-100 V, meeting the operating voltage requirements of most common SiPM models. The experimental results show that in the temperature range of -20-40 ℃. The maximum peak sites of 662, 1 173, 1 332, and 59.5 keV full-energy peaks are 515.9, 915.8, 1 041.0, and 43.1, and the minimum peak sites are 507.1, 899.0, 1 022.9, and 43.1. The maximum positive drifts are 4.6, 7.8, 8.1 and 0.5 lanes and the maximum negative drifts are 4.2, 8.7, 9.8 and 0.5 lanes respectively. Compared to the 662 keV for 137Cs, 1 173 and 1 332 keV for 60Co and 59.5 keV for 241Am peak sites measured without temperature compensation, the average drifts of the peak sites with SiPM-only temperature compensation are reduced from 45.34%, 45.13%, 44.98%, and 43.85% to 23.68%, 23.67%, 23.68% and 18.30%. The temperature effect of the scintillation crystal has to be taken into account for the temperature compensation of the whole detector. After the overall temperature compensation of the SiPM-GAGG(Ce) detector, the average drift rates of 662 keV for 137Cs, 1 173 keV and 1 332 keV for 60Co and 59.5 keV for 241Am peak channel sites are reduced to 0.37%, 0.37%, 0.36% and 0.57%, which is a significant compensation effect. In the absence of temperature compensation, the 137Cs energy resolution varies from 8.08% at -20 ℃ to 14.58% at 40 ℃. After compensating for the temperature effect of the SiPM-GAGG(Ce) detector, the137Cs energy resolution changes from 8.36% at -20 ℃ to 9.29% at 40 ℃. The stability of the energy resolution is significantly improved. The temperature compensation system has the advantages of low noise, small size and freely customisable temperature characteristic curves. It effectively solves the problem of significant differences in the driving voltage of SiPM from different manufacturers and the compensation of temperature effects after coupling the 8×8 SiPM array with Φ2 in×2 in GAGG(Ce) crystals, and significantly improves the stability of the γ spectrometry system.

     

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