Aldosary Ghada, Safigholi Habib, Song William, Seuntjens Jan, Sarfehnia Arman
Department of Medical Physics, Cedars Cancer Centre, McGill University Health Centre (Glen Site), DS1 7141, 1001 boul. Decarie, Montreal, Quebec H4A 3J1, Canada.
Department of Medical Physics, Odette Cancer Centre, Sunnybrook Health Sciences Centre, Room TG276, T wing, 2075 Bayview Avenue, Toronto, Ontario M4N 3M5, Canada.
Phys Med. 2017 Mar;35:102-109. doi: 10.1016/j.ejmp.2017.01.019. Epub 2017 Feb 12.
In this work, the response of Farmer-type ionization chambers fitted with high atomic number (Z) walls is studied, and results of the effects of such walls on polarity and ion recombination correction factors in both continuous and pulsed beams are presented. Measurements were made in a continuous Co-60 beam and a pulsed 6MV linac beam using an Exradin-A12 ionization chamber fitted with the manufacturer's C-552 plastic wall, as well as geometrically identical walls made from aluminum, copper and molybdenum. The bias voltage was changed between 10values (range: +50 to +560V). Ion recombination was determined from Jaffé plots and by using the "two-voltage technique". The saturation charge measured with each chamber wall was extrapolated from Jaffé plots. Additionally, the effect of different wall materials on chamber response was studied using MCNP simulations. Results showed that the polarity correction factor is not significantly affected by changes in chamber wall material (within 0.1%). Furthermore, although the saturation charges greatly vary with each chamber wall material, and charge multiplication increases for higher atomic number wall materials, the standard methods of calculating ion recombination yielded results that differed by only 0.2%. Therefore, polarity and ion recombination correction factors are not greatly affected by the chamber wall material. The experimental saturation charges for all the different wall materials agreed well within the uncertainty with MCNP simulations. The breakdown of the linear relationship in Jaffé plots that was previously reported to exist for conventional chamber walls was also observed with the different wall materials.
在这项工作中,研究了配备高原子序数(Z)壁的Farmer型电离室的响应,并给出了这种壁对连续和脉冲束中极性和离子复合校正因子影响的结果。使用配备制造商C-552塑料壁的Exradin-A12电离室,以及由铝、铜和钼制成的几何形状相同的壁,在连续Co-60束和脉冲6MV直线加速器束中进行了测量。偏置电压在10个值(范围:+50至+560V)之间变化。通过Jaffé图并使用“双电压技术”确定离子复合。用每个电离室壁测量的饱和电荷从Jaffé图中推断得出。此外,使用MCNP模拟研究了不同壁材料对电离室响应的影响。结果表明,极性校正因子不受电离室壁材料变化的显著影响(在0.1%以内)。此外,尽管饱和电荷随每种电离室壁材料有很大变化,并且对于原子序数较高的壁材料电荷倍增增加,但计算离子复合的标准方法得出的结果仅相差0.2%。因此,极性和离子复合校正因子不受电离室壁材料的很大影响。所有不同壁材料的实验饱和电荷在不确定性范围内与MCNP模拟结果吻合良好。对于不同的壁材料,也观察到了先前报道的传统电离室壁在Jaffé图中存在的线性关系的破坏。