首页> 外文会议>IEEE International Solid-State Circuits Conference >An 8#x00D7;16-pixel 92kSPAD time-resolved sensor with on-pixel 64ps 12b TDC and 100MS/s real-time energy histogramming in 0.13#x00B5;m CIS technology for PET/MRI applications
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An 8#x00D7;16-pixel 92kSPAD time-resolved sensor with on-pixel 64ps 12b TDC and 100MS/s real-time energy histogramming in 0.13#x00B5;m CIS technology for PET/MRI applications

机译:一个8×16像素的92kSPAD时间分辨传感器,具有0.13µm CIS技术的像素上64ps 12b TDC和100MS / s实时能量直方图,适用于PET / MRI应用

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Positron-Emission Tomography (PET) is a nuclear imaging technique that provides functional 3-dimensional images of the body, finding its key applications in clinical oncology and brain-function analyses. The typical PET scanner is composed of a ring of scintillator crystals that absorb gamma rays and emit photons as a result, coupled to photon-sensing devices. The photons hit the sensors with a certain spread in space and time, depending on the material and geometry of the crystals. The sensors must then estimate the energy, the time of arrival (ToA), and the axial position of incoming gamma rays. Most commercially available scanners use photomultiplier tubes (PMTs), which are sensitive to magnetic fields, as the sensing element, making the integration of these systems with Magnetic-Resonance Imaging (MRI) impossible. A significant amount of research has focused on replacing PMTs with solid-state detectors, such as Silicon photomultipliers (SiPMs) [1], which can be integrated with MRI while maintaining the high-sensitivity of PMTs.
机译:正电子发射断层扫描(PET)是一种核成像技术,可提供人体的功能性3维图像,并在临床肿瘤学和脑功能分析中找到了关键应用。典型的PET扫描仪由闪烁体晶体环组成,该晶体吸收伽马射线并因此发射光子,并耦合到光子传感设备。根据晶体的材料和几何形状,光子以一定的时空分布撞击传感器。然后,传感器必须估算能量,到达时间(ToA)和入射伽马射线的轴向位置。大多数商用扫描仪都使用对磁场敏感的光电倍增管(PMT)作为传感元件,因此无法将这些系统与磁共振成像(MRI)集成在一起。大量研究集中在用固态检测器代替PMT,例如硅光电倍增管(SiPM)[1],该检测器可以与MRI集成在一起,同时保持PMT的高灵敏度。

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