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用于计算机断层扫描的市售光激励发光剂量测定系统的特性描述。

Characterization of a commercially-available, optically-stimulated luminescent dosimetry system for use in computed tomography.

机构信息

Tufts Medical Center, Department of Radiology, 800 Washington St., Box 299, Boston, MA 02111, USA.

出版信息

Health Phys. 2011 Sep;101(3):299-310. doi: 10.1097/HP.0b013e31820f8e0e.

DOI:10.1097/HP.0b013e31820f8e0e
PMID:21799346
Abstract

Optically-stimulated luminescent (OSL) nanoDot dosimeters, commercially available from Landauer, Inc. (Glenwood, IL), were assessed for use in computed tomography (CT) for erasure and reusability, linearity and reproducibility of response, and angular and energy response in different scattering conditions. Following overnight exposure to fluorescent room light, the residual signal on the dosimeters was 2%. The response of the dosimeters to identical exposures was consistent, and reported doses were within 4% of each other. The dosimeters responded linearly with dose up to 1 Gy. The dosimeter response to the CT beams decreased with increased tube voltage, showing up to a -16% difference when compared to a 0.6-cm(3) NIST-traceable calibrated ionization chamber for a 135 kVp CT beam. The largest range in percent difference in dosimeter response to scatter at central and peripheral positions inside CTDI phantoms was 14% at 80 kVp CT tube voltage, when compared to the ionization chamber. The dosimeters responded uniformly to x-ray tube angle over the ranges of increments of 0° to 75° and 105° to 180° when exposed in air, and from 0° to 360° when exposed inside a CTDI phantom. While energy and scatter correction factors should be applied to dosimeter readings for the purpose of determining absolute doses, these corrections are straightforward but depend on the accuracy of the ionization chamber used for cross-calibration. The linearity and angular responses, combined with the ability to reuse the dosimeters, make this OSL system an excellent choice for clinical CT dose measurements.

摘要

光学刺激发光 (OSL) 纳米点剂量计,可从 Landauer, Inc.(伊利诺伊州格伦伍德)商业获得,评估其在计算机断层扫描 (CT) 中的擦除和可重复使用性、响应的线性和重现性以及不同散射条件下的角度和能量响应。在荧光室内光下过夜暴露后,剂量计上的剩余信号为 2%。剂量计对相同暴露的响应一致,报告的剂量彼此相差在 4%以内。剂量计在高达 1 Gy 的剂量下呈线性响应。随着管电压的增加,剂量计对 CT 射线的响应降低,与 0.6cm(3)NIST 可追踪校准电离室相比,135 kVp CT 射线的差异高达-16%。在 80 kVp CT 管电压下,与电离室相比,在 CTDI 体模内部中心和外围位置的散射下,剂量计响应的百分比差异最大范围为 14%。当在空气中以 0°至 75°和 105°至 180°的增量曝光时,以及当在 CTDI 体模内部以 0°至 360°的增量曝光时,剂量计对 X 射线管角度的响应均匀。虽然为了确定绝对剂量,应该对剂量计读数应用能量和散射校正因子,但这些校正因子很简单,但取决于用于交叉校准的电离室的准确性。线性和角度响应,加上可重复使用剂量计的能力,使这个 OSL 系统成为临床 CT 剂量测量的绝佳选择。

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