Heemskerk Jan W T, Westra Albert H, Linotte Peter M, Ligtvoet Kees M, Zbijewski Wojciech, Beekman Freek J
Department of Nuclear Medicine, Image Sciences Institute, University Medical Center Utrecht, Room STR 5.203, Universiteitsweg 100, 3584 CG Utrecht, The Netherlands.
Phys Med Biol. 2007 Apr 21;52(8):N149-62. doi: 10.1088/0031-9155/52/8/N01. Epub 2007 Mar 23.
Charge-coupled devices (CCDs) coupled to scintillation crystals can be used for high-resolution imaging with x-rays and gamma rays. When the CCD images can be read out fast enough, the energy and interaction position of individual gamma quanta can be estimated by a real-time image analysis of the scintillation light flashes ('photon-counting mode'). The electron-multiplying CCD (EMCCD) is well suited for fast read out, since even at high frame rates it has extremely low read-out noise. Back-illuminated (BI) EMCCDs have much higher quantum efficiency than front-illuminated (FI) EMCCDs. Here we compare the spatial and energy resolution of gamma cameras based on FI and BI EMCCDs. The CCDs are coupled to a 1000 microm thick columnar CsI(Tl) crystal for the purpose of Tc-99m and I-125 imaging. Intrinsic spatial resolutions of 44 microm for I-125 and 49 microm for Tc-99m were obtained when using a BI EMCCD, which is an improvement by a factor of about 1.2-2 over the FI EMCCD. Furthermore, in the energy spectrum of the BI EMCCD, the I-125 signal could be clearly separated from the background noise, which was not the case for the FI EMCCD. The energy resolution of a BI EMCCD for Tc-99m was estimated to be approximately 36 keV, full width at half maximum, at 141 keV. The excellent results for the BI EMCCD encouraged us to investigate the cooling requirements for our setup. We have found that for the BI EMCCD, the spatial and energy resolution, as well as image noise, remained stable over a range of temperatures from -50 degrees C to -15 degrees C. This is a significant advantage over the FI EMCCD, which suffered from loss of spatial and especially energy resolution at temperatures as low as -40 degrees C. We conclude that the use of BI EMCCDs may significantly improve the imaging capabilities and the cost efficiency of CCD-based high-resolution gamma cameras.
与闪烁晶体耦合的电荷耦合器件(CCD)可用于X射线和伽马射线的高分辨率成像。当CCD图像能够足够快地读出时,通过对闪烁光脉冲进行实时图像分析(“光子计数模式”),可以估算出单个伽马量子的能量和相互作用位置。电子倍增CCD(EMCCD)非常适合快速读出,因为即使在高帧率下,它也具有极低的读出噪声。背照式(BI)EMCCD的量子效率比前照式(FI)EMCCD高得多。在此,我们比较了基于FI和BI EMCCD的伽马相机的空间分辨率和能量分辨率。为了进行Tc-99m和I-125成像,将CCD与一块1000微米厚的柱状碘化铯(铊)晶体耦合。使用BI EMCCD时,I-125的固有空间分辨率为44微米,Tc-99m的固有空间分辨率为49微米,比FI EMCCD提高了约1.2至2倍。此外,在BI EMCCD的能谱中,I-125信号能够与背景噪声清晰分离,而FI EMCCD则并非如此。对于Tc-99m,BI EMCCD在141 keV处的能量分辨率估计约为36 keV(半高宽)。BI EMCCD的出色结果促使我们研究该装置的冷却要求。我们发现,对于BI EMCCD,在-50℃至-15℃的温度范围内,空间分辨率、能量分辨率以及图像噪声均保持稳定。这相较于FI EMCCD是一个显著优势,后者在低至-40℃的温度下会出现空间分辨率尤其是能量分辨率的损失。我们得出结论,使用BI EMCCD可能会显著提高基于CCD的高分辨率伽马相机的成像能力和成本效益。