Wendisch M, Freudenberg R, Drechsel J, Runge R, Wunderlich G, Kotzerke J
Klinik und Poliklinik für Nuklearmedizin, Universitätsklinikum Carl Gustav Carus, Technische Universität Dresden, Germany.
Nuklearmedizin. 2010;49(4):154-60. doi: 10.3413/nukmed-0300. Epub 2010 May 21.
In addition to gamma radiation of 140 keV 99mTc emits during the transition to 99Tc electrons of low energy and tiny path-lengths. These Auger electrons cannot be utilized in diagnostic procedures. However, they were discussed frequently for therapeutic application. Hitherto proof of effect of the Auger electrons from 99mTc is missing which is supplied now in an in vitro-system in comparison to beta-emitter 131I.
The thyroid cell line PCCl3 (sodium iodide symporter (NIS)-positive) was incubated with 131I-sodium iodide (131I) or 99mTc-pertechnetate (99mTc) in presence or absence of perchlorate. For comparison the amount of radioactivity was adjusted to obtain the same dose from extracellular irradiation for both radionuclides. The colony forming assay detects the clonogenic cell survival as surviving fraction. In addition, intracellular radionuclide uptake was quantified.
Dose effect curves were established for 131I and 99mTc for variable extra- and intracellular distribution of the radioactivity. In presence of perchlorate no cellular uptake of radioactivity was detectable. Survival curves were largely comparable confirming the dosimetric calculations. In absence of perchlorate cellular radiotracer uptake varied from 1.39% (131I) to 1.90% 99mTc). Effects on survival were twice for the beta-emitter and ten-fold higher for 99mTc.
Intracellular uptake of 131I and 99mTc increases DNA-damage compared to strict extracellular radiotracer distribution which was demonstrated by means of colony forming assay. Increasing radiotoxicity from intracellular 99mTc is explained most likely by increased dose deposition in cellular structures due to Auger- and conversion-electrons of low range and high local energy deposition.
除了在向99Tc跃迁过程中140keV的γ辐射外,99mTc还会发射低能量和微小路径长度的电子。这些俄歇电子无法用于诊断程序。然而,它们在治疗应用方面经常被讨论。迄今为止,99mTc产生的俄歇电子的效果证据尚缺,现通过体外系统与β发射体131I进行比较来提供此证据。
甲状腺细胞系PCCl3(钠碘同向转运体(NIS)阳性)在有或无高氯酸盐存在的情况下,用131I-碘化钠(131I)或99mTc-高锝酸盐(99mTc)孵育。为作比较,调整放射性活度的量,以使两种放射性核素从细胞外照射获得相同剂量。集落形成试验将克隆形成细胞存活率检测为存活分数。此外,对细胞内放射性核素摄取进行定量。
针对131I和99mTc建立了放射性活度在细胞外和细胞内不同分布情况下的剂量效应曲线。在有高氯酸盐存在时,未检测到细胞对放射性活度的摄取。存活曲线在很大程度上具有可比性,证实了剂量测定计算结果。在无高氯酸盐时,细胞放射性示踪剂摄取量从1.39%(131I)到1.90%(99mTc)不等。β发射体对存活的影响是其两倍,而99mTc的影响则高十倍。
与严格的细胞外放射性示踪剂分布相比,131I和99mTc在细胞内的摄取增加了DNA损伤,这通过集落形成试验得到了证实。细胞内99mTc放射性毒性增加最可能的解释是,由于低射程和高局部能量沉积的俄歇电子及转换电子导致细胞结构中的剂量沉积增加。