导管血管内近距离放射治疗时,偏离中心对沿血管及血管周围剂量均匀性的影响

Ravinder Nath, Ning Yue
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引用次数: 1

摘要

目的:在血管内近距离放射治疗中,光子或发射体通常呈线性排列,以便治疗长度在几厘米范围内的血管。对于线源,剂量均匀性和血管各组成部分接受的剂量范围不仅取决于治疗中使用的放射性核素的类型,而且还取决于放射源相对于血管壁的几何位置。本研究的目的是研究血管周围的剂量均匀性,以及腔内不同光子和β发射器偏离中心的变化对均匀性的影响。材料与方法在不同半径的圆柱形血管上计算剂量分布。研究了192Ir、125I、103Pd、188Re、32P和90Y/Sr的放射源。所有的光源都假定为一条线的形式,长度为2厘米。放射源在空间某一点产生的剂量率是通过对相应的放射性核素在2厘米长的放射性线上的点剂量率核积分来计算的。利用蒙特卡罗辐射输运模拟计算了点剂量率核。对同心圆和非同心圆放射源位置进行了剂量学计算。偏移对剂量学的影响用两个新定义的量LDU和ADU来表征:LDU描述沿血管的纵向剂量均匀性,ADU描述沿血管的方位角剂量均匀性,即血管周围剂量与预期给药剂量的偏差。结果纵向剂量均匀性随离中心距离变化不显著。随着离中心距离的增加,血管周围方位剂量均匀性变差。非同心发射体的ADU比光子发射体差。例如,当离中心距离为1 mm,径向距离为1.5 mm时,192Ir、125I、103Pd、90Y/Sr、188Re、32P源在中央横切面血管周围的剂量范围(标准化为同心圆条件下的相应剂量)分别为0.55 ~ 3.3、0.56 ~ 3.3、0.53 ~ 3.4、0.43 ~ 6.0、0.38 ~ 4.3、0.31 ~ 4.7。然而,由于光子发射体偏离中心,似乎存在一个剂量不足的下限(约为期望递送剂量的40%)。当辐照源长度大于或等于20 mm时,ADU和LDU几乎与辐照源长度无关。结论建立了线性辐照源沿血管和血管周围剂量均匀性的广义表达式,并用于研究不同类型放射性核素的纵向和方位剂量均匀性。尽管同心发射体沿血管提供均匀的剂量覆盖,但与光子发射体相比,非同心发射体在血管周围产生更大的剂量偏差和更差的剂量均匀性。偏离中心对β和光子发射器近端血管壁的剂量都显著增加;然而,对于高能光子发射器来说,由于偏离中心导致的远端剂量不足在一定程度上受到限制。低能光子发射体(103Pd)偏离中心效应的幅度小于β发射体,但大于高能光子发射体(125I和192Ir)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Effects of off-centering on dose uniformity along and around blood vessels undergoing catheter-based intravascular brachytherapy

Purpose

In intravascular brachytherapy, either photon or beta emitters are often used in a linear arrangement so that blood vessels of lengths in the range of several centimeters can be treated. With a line source, the dose uniformity and the range of doses that various components of the blood vessels receive depend not only on the type of radionuclides used in the treatment but also on the geometric position of radioactive source relative to the blood vessel walls. The aim of this study is to investigate the dose uniformity around the blood vessel and the effects on the uniformity due to the changes of the off-centering of different photon and beta emitters within the lumen.

Materials and methods

Dose distributions were calculated on a cylindrical blood vessel of various radii. The radioactive sources of 192Ir, 125I, 103Pd, 188Re, 32P, and 90Y/Sr were studied. All the sources were assumed to be in the form of a line and had a length of 2 cm. The dose rate at a point in space produced by a radioactive source was computed by integrating the point dose rate kernel of the corresponding radionuclide over the 2-cm-long radioactive line. The point dose rate kernel was computed with Monte Carlo simulation of radiation transport. Dosimetric calculations were performed for both concentric and nonconcentric radioactive line source locations. Off-centering effects on the dosimetry were characterized with two newly defined quantities LDU and ADU: LDU describes the longitudinal dose uniformity along blood vessels and ADU describes the azimuthal dose uniformity, i.e., the dose deviation from the expected delivery dose around blood vessels.

Results

The longitudinal dose uniformity did not change significantly with the off-center distance. The azimuthal dose uniformity around the blood vessel deteriorated as the off-center distance increased. The ADU was worse for nonconcentric beta emitters than the photon emitters. For example, if the off-center distance was 1 mm and the radial distance was 1.5 mm, the range of dose around the blood vessel on the central transverse plane (normalized to the corresponding dose under the concentric condition) was from 0.55 to 3.3, 0.56 to 3.3, 0.53 to 3.4, 0.43 to 6.0, 0.38 to 4.3, and 0.31 to 4.7 for 192Ir, 125I, 103Pd, 90Y/Sr, 188Re, and 32P sources, respectively. However, it appeared that there existed a lower limit of underdosing (about 40% of desired delivery dose) caused by the off-centering for the photon emitters. It was also found that both ADU and LDU became almost independent of source length when the length was longer than or equal to 20 mm.

Conclusions

A generalized formalism for expressing the dose uniformity along and around blood vessels generated with a linear source was developed and used to study the longitudinal and azimuthal dose uniformity for different types of radionuclides. Although concentric beta emitters provide uniform dose coverage along blood vessels, nonconcentric beta emitters produced larger dose deviations and worse dose uniformity around the blood vessels than photon emitters. The off-centering introduced significantly higher dose on proximal vessel walls for both beta and photon emitters; however, the underdosing at distal points due to off-centering was somewhat limited for the high-energy photon emitters. The magnitude of off-centering effects for the low-energy photon emitters (103Pd) was less than that for beta emitters but more than that for higher energy photon emitters (125I and 192Ir).

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