Avilés Lucas P, Dance D R, Castellano I A, Vañó E
Physics Department, The Royal Marsden NHS Trust, Fulham Road. London SW3 6JJ, UK.
Radiat Prot Dosimetry. 2005;114(1-3):317-20. doi: 10.1093/rpd/nch522.
The purpose of this work was to develop a method for estimating the patient peak entrance surface air kerma from measurements using a pencil ionisation chamber on dosimetry phantoms exposed in a computed tomography (CT) scanner. The method described is especially relevant for CT fluoroscopy and CT perfusion procedures where the peak entrance surface air kerma is the risk-related quantity of primary concern. Pencil ionisation chamber measurements include scattered radiation, which is outside the primary radiation field, and that must be subtracted in order to derive the peak entrance surface air kerma. A Monte Carlo computer model has therefore been used to calculate correction factors, which may be applied to measurements of the CT dose index obtained using a pencil ionisation chamber in order to estimate the peak entrance surface air kerma. The calculations were made for beam widths of 5, 7, 10 and 20 mm, for seven positions of the phantom, and for the geometry of a GE HiSpeed CT/i scanner. The program was validated by comparing measurements and calculations of CTDI for various vertical positions of the phantom and by directly estimating the peak ESAK using the program. Both validations showed agreement within statistical uncertainties (standard deviation of 2.3% or less). For the GE machine, the correction factors vary by approximately 10% with slice width for a fixed phantom position, being largest for the 20 mm beam width, and at that beam width range from 0.87 when the phantom surface is at the isocentre to 1.23 when it is displaced vertically by 24 cm.
这项工作的目的是开发一种方法,通过在计算机断层扫描(CT)扫描仪中对剂量学体模进行测量,使用笔形电离室来估计患者体表空气比释动能峰值。所描述的方法对于CT透视和CT灌注程序尤为重要,因为体表空气比释动能峰值是主要关注的与风险相关的量。笔形电离室测量包括初级辐射场外的散射辐射,为了得出体表空气比释动能峰值,必须将其减去。因此,使用蒙特卡罗计算机模型来计算校正因子,该校正因子可应用于使用笔形电离室获得的CT剂量指数测量,以估计体表空气比释动能峰值。针对5、7、10和20毫米的束宽、体模的七个位置以及GE HiSpeed CT/i扫描仪的几何结构进行了计算。通过比较体模不同垂直位置的CTDI测量值和计算值,并使用该程序直接估计体表空气比释动能峰值来验证该程序。两次验证均显示在统计不确定度(标准偏差为2.3%或更低)范围内一致。对于GE机器,对于固定的体模位置,校正因子随切片宽度变化约10%,在20毫米束宽时最大,在该束宽下,当体模表面位于等中心时校正因子为0.87,当垂直位移24厘米时为1.23。