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POSITRON EMISSION TOMOGRAPHY WITHIN A MAGNETIC FIELD USING PHOTOMULTIPLIER TUBES AND LIGHTGUIDES

机译:使用光电倍增管和光导在磁场中进行正电子发射断层扫描

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摘要

The spatial resolution of positron emission tomography (PET) improves when positron annihilation takes place in a strong magnetic field. In a magnetic field, the Lorentz force restricts positron range perpendicular to the field. Since positron annihilation occurs closer to its point of origin, the positron annihilation point spread function decreases. This was verified experimentally by measuring the spread function of positron annihilation from a 500 mm Ge-68 bead imbedded in tissue-equivalent wax. At 5 T the spread function full width at half maximum (FWHM) and the full width at tenth maximum (FWTM) decrease by a factor of 1.42 and 2.09, respectively. Two Nar(TI) scintillation crystals that interface to a pair of photomultiplier tubes (PMTS) through long lightguides detect positron annihilation at zero field and 5.0 T. Photomultiplier tubes, inoperable in strong magnetic fields, are functional if lightguides bring the photons produced by scintillators within the field to a minimal magnetic field. These tests also demonstrate techniques necessary for combining magnetic resonance imaging (MRI) and PET into one scanner. [References: 11]
机译:当在强磁场中进行正电子an没时,正电子发射断层扫描(PET)的空间分辨率会提高。在磁场中,洛伦兹力限制了垂直于磁场的正电子范围。由于正电子an灭发生在其起点附近,因此正电子an灭点扩展函数减小。通过测量嵌入到组织等效蜡中的500 mm Ge-68珠子中正电子an灭的扩散函数,可以通过实验验证这一点。在5 T时,扩展函数的半高全宽(FWHM)和十分大全宽(FWTM)分别减小了1.42和2.09倍。通过长光导与一对光电倍增管(PMTS)接合的两个Nar(TI)闪烁晶体可检测零场和5.0 T时的正电子ni灭。如果光导将闪烁体产生的光子带入,则在强磁场中不可操作的光电倍增管将起作用。磁场内的磁场最小。这些测试还演示了将磁共振成像(MRI)和PET组合到一个扫描仪中所需的技术。 [参考:11]

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