Crump Institute for Molecular Imaging, Department of Medical and Molecular Pharmacology, David Geffen School of Medicine at UCLA, Los Angeles, CA, USA.
Phys Med Biol. 2009 Nov 21;54(22):6757-71. doi: 10.1088/0031-9155/54/22/001. Epub 2009 Oct 21.
It has been observed that microfluidic chips used for synthesizing (18)F-labeled compounds demonstrate visible light emission without nearby scintillators or fluorescent materials. The origin of the light was investigated and found to be consistent with the emission characteristics from Cerenkov radiation. Since (18)F decays through the emission of high-energy positrons, the energy threshold for beta particles, i.e. electrons or positrons, to generate Cerenkov radiation was calculated for water and polydimethylsiloxane (PDMS), the most commonly used polymer-based material for microfluidic chips. Beta particles emitted from (18)F have a continuous energy spectrum, with a maximum energy that exceeds this energy threshold for both water and PDMS. In addition, the spectral characteristics of the emitted light from (18)F in distilled water were also measured, yielding a broad distribution from 300 nm to 700 nm, with higher intensity at shorter wavelengths. A photograph of the (18)F solution showed a bluish-white light emitted from the solution, further suggesting Cerenkov radiation. In this study, the feasibility of using this Cerenkov light emission as a method for quantitative measurements of the radioactivity within the microfluidic chip in situ was evaluated. A detector previously developed for imaging microfluidic platforms was used. The detector consisted of a charge-coupled device (CCD) optically coupled to a lens. The system spatial resolution, minimum detectable activity and dynamic range were evaluated. In addition, the calibration of a Cerenkov signal versus activity concentration in the microfluidic chip was determined. This novel method of Cerenkov radiation measurements will provide researchers with a simple yet robust quantitative imaging tool for microfluidic applications utilizing beta particles.
已经观察到,用于合成 (18)F 标记化合物的微流控芯片在没有附近的闪烁体或荧光材料的情况下表现出可见光发射。研究了光的起源,发现它与切伦科夫辐射的发射特性一致。由于 (18)F 通过发射高能正电子而衰变,因此计算了水和聚二甲基硅氧烷 (PDMS)(最常用于微流控芯片的聚合物基材料)中产生切伦科夫辐射的β粒子的能量阈值,即电子或正电子。从 (18)F 发射的β粒子具有连续的能谱,其最大能量超过了水和 PDMS 的这一能量阈值。此外,还测量了 (18)F 在蒸馏水发射的光的光谱特性,得到了一个从 300nm 到 700nm 的宽分布,在较短波长处强度更高。(18)F 溶液的照片显示溶液发出蓝白色光,进一步表明存在切伦科夫辐射。在这项研究中,评估了将这种切伦科夫光发射用作原位定量测量微流控芯片内放射性的可行性。使用了先前为微流控平台成像开发的检测器。评估了检测器的空间分辨率、最小可检测活性和动态范围。此外,还确定了微流控芯片中切伦科夫信号与活性浓度的校准。这种新的切伦科夫辐射测量方法将为研究人员提供一种简单而强大的定量成像工具,用于利用β粒子的微流控应用。