PO61

Fada Guan, Emily Draeger, David Carlson, Zhe Chen, Christopher Tien
{"title":"PO61","authors":"Fada Guan, Emily Draeger, David Carlson, Zhe Chen, Christopher Tien","doi":"10.1016/j.brachy.2023.06.162","DOIUrl":null,"url":null,"abstract":"Purpose In the conventional fractionation schemes of high-dose-rate (HDR) brachytherapy, the intra-fractional and inter-fractional DNA damage repair and repopulation of tumor cells are neglected in calculating the biologically effective dose (BED). This may result in inaccurate model prediction of the theoretical tumor control probability (TCP). Notwithstanding, current prostate brachytherapy prescriptions may still be large enough to theoretically overcome these effects, among others. The purpose of this study was to recalculate the theoretical TCP, accounting for intrafraction DNA damage repair and 192Ir source decay for prostate cancer treated using HDR brachytherapy as the monotherapy, compared against common 1-, 2-, and 9-fraction prescription schemes. Materials and Methods We incorporated the Lea-Catcheside dose protraction factor g, the effective tumor doubling time Td, the total elapsed time of the treatment course T, and the onset or lag time of cell repopulation Tk, into the full-form BED calculation, in contrast to the simple form BED which only includes the total dose, dose per fraction and α/β. The Poisson model relating the surviving fraction and the number of tumor clonogens (K) was used to calculate TCP. The parameter set α = 0.15 Gy-1, α/β = 3.1 Gy, τ = 0.27 h (DNA damage repair half time), Td = 42 days, and Tk = 0 was used for the full-form BED calculation. K = 1.1 × 107 from the high-risk group was used in the TCP calculation. The new 192Ir source (40,700 U, 10 Ci, 1.27 Gy/min) and the 90-day source (17,470 U, 4.3 Ci, 0.55 Gy/min) were used to investigate the source decay effect on TCP. Three different fractionation schemes n = 1, 2, and 9 fraction(s) were studied. Simple BED, full-form BED (both 10 Ci and 4.3 Ci), TCP50 (total dose at TCP = 50%), and TCP90 (total dose at TCP = 90%) were calculated for each setup. 1 x 21 Gy, 2 x 13.5 Gy, and 9 x 6 Gy prescriptions were selected to evaluate the robustness of different fractionation schemes on TCP impacted by DNA damage repair and source decay. Results TCP50 and TCP90 using the simple BED, the full-form BED at 10 Ci and 4.3 Ci were calculated. In the single-fraction group, TCP50 = 17.0, 18.6, and 21.2 Gy, and TCP90 = 18.0, 19.9, and 22.8 Gy. In the 2-fraction group, TCP50 = 23.3, 24.7, and 26.8 Gy, and TCP90 = 24.7, 26.3, and 28.7 Gy. In the 9-fraction group, TCP50 = 43.3, 44.3, and 45.6 Gy, and TCP90 = 46.3, 47.4, and 48.9 Gy. For 1 × 21 Gy, the simple BED and full-form BED (10 Ci and 4.3 Ci) = 163.3, 134.8, and 109.0 Gy, and TCP = 99.9%, 98.2%, and 41.9%. For 2 × 13.5 Gy, the simple BED and full-from BED (10 Ci and 4.3 Ci) = 144.6, 128.5, and 112.0 Gy, and TCP = 99.6%, 95.4%, and 57.4%. For 9 × 6 Gy, the simple BED and full-from BED (10 Ci and 4.3 Ci) = 158.5, 151.4, and 143.4 Gy, and TCP = 99.9%, 99.9%, and 99.5%. In general, we have observed: (1) using the simple BED overestimated the TCP compared to the full-form BED, (2) with the source decay, a higher total dose was needed to achieve the same level of TCP, (3) using the hypo-fractionation saved total dose and total irradiation time to achieve the same TCP, but (4) using the hyper-fractionation can dampen the effects of DNA damage repair and source decay on TCP. Conclusions The changes in BED introduced by the Lea-Catcheside dose protraction factor into our TCP model were most significant for deliveries with a long treatment time and/or a decayed source. Current prescriptions for 1, 2, and 9 fraction(s) are adequate to reach TCP of at least 41.9%, 57.4%, and 99.5%. In the conventional fractionation schemes of high-dose-rate (HDR) brachytherapy, the intra-fractional and inter-fractional DNA damage repair and repopulation of tumor cells are neglected in calculating the biologically effective dose (BED). This may result in inaccurate model prediction of the theoretical tumor control probability (TCP). Notwithstanding, current prostate brachytherapy prescriptions may still be large enough to theoretically overcome these effects, among others. The purpose of this study was to recalculate the theoretical TCP, accounting for intrafraction DNA damage repair and 192Ir source decay for prostate cancer treated using HDR brachytherapy as the monotherapy, compared against common 1-, 2-, and 9-fraction prescription schemes. We incorporated the Lea-Catcheside dose protraction factor g, the effective tumor doubling time Td, the total elapsed time of the treatment course T, and the onset or lag time of cell repopulation Tk, into the full-form BED calculation, in contrast to the simple form BED which only includes the total dose, dose per fraction and α/β. The Poisson model relating the surviving fraction and the number of tumor clonogens (K) was used to calculate TCP. The parameter set α = 0.15 Gy-1, α/β = 3.1 Gy, τ = 0.27 h (DNA damage repair half time), Td = 42 days, and Tk = 0 was used for the full-form BED calculation. K = 1.1 × 107 from the high-risk group was used in the TCP calculation. The new 192Ir source (40,700 U, 10 Ci, 1.27 Gy/min) and the 90-day source (17,470 U, 4.3 Ci, 0.55 Gy/min) were used to investigate the source decay effect on TCP. Three different fractionation schemes n = 1, 2, and 9 fraction(s) were studied. Simple BED, full-form BED (both 10 Ci and 4.3 Ci), TCP50 (total dose at TCP = 50%), and TCP90 (total dose at TCP = 90%) were calculated for each setup. 1 x 21 Gy, 2 x 13.5 Gy, and 9 x 6 Gy prescriptions were selected to evaluate the robustness of different fractionation schemes on TCP impacted by DNA damage repair and source decay. TCP50 and TCP90 using the simple BED, the full-form BED at 10 Ci and 4.3 Ci were calculated. In the single-fraction group, TCP50 = 17.0, 18.6, and 21.2 Gy, and TCP90 = 18.0, 19.9, and 22.8 Gy. In the 2-fraction group, TCP50 = 23.3, 24.7, and 26.8 Gy, and TCP90 = 24.7, 26.3, and 28.7 Gy. In the 9-fraction group, TCP50 = 43.3, 44.3, and 45.6 Gy, and TCP90 = 46.3, 47.4, and 48.9 Gy. For 1 × 21 Gy, the simple BED and full-form BED (10 Ci and 4.3 Ci) = 163.3, 134.8, and 109.0 Gy, and TCP = 99.9%, 98.2%, and 41.9%. For 2 × 13.5 Gy, the simple BED and full-from BED (10 Ci and 4.3 Ci) = 144.6, 128.5, and 112.0 Gy, and TCP = 99.6%, 95.4%, and 57.4%. For 9 × 6 Gy, the simple BED and full-from BED (10 Ci and 4.3 Ci) = 158.5, 151.4, and 143.4 Gy, and TCP = 99.9%, 99.9%, and 99.5%. In general, we have observed: (1) using the simple BED overestimated the TCP compared to the full-form BED, (2) with the source decay, a higher total dose was needed to achieve the same level of TCP, (3) using the hypo-fractionation saved total dose and total irradiation time to achieve the same TCP, but (4) using the hyper-fractionation can dampen the effects of DNA damage repair and source decay on TCP. The changes in BED introduced by the Lea-Catcheside dose protraction factor into our TCP model were most significant for deliveries with a long treatment time and/or a decayed source. Current prescriptions for 1, 2, and 9 fraction(s) are adequate to reach TCP of at least 41.9%, 57.4%, and 99.5%.","PeriodicalId":93914,"journal":{"name":"Brachytherapy","volume":"44 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2023-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Brachytherapy","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1016/j.brachy.2023.06.162","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

Purpose In the conventional fractionation schemes of high-dose-rate (HDR) brachytherapy, the intra-fractional and inter-fractional DNA damage repair and repopulation of tumor cells are neglected in calculating the biologically effective dose (BED). This may result in inaccurate model prediction of the theoretical tumor control probability (TCP). Notwithstanding, current prostate brachytherapy prescriptions may still be large enough to theoretically overcome these effects, among others. The purpose of this study was to recalculate the theoretical TCP, accounting for intrafraction DNA damage repair and 192Ir source decay for prostate cancer treated using HDR brachytherapy as the monotherapy, compared against common 1-, 2-, and 9-fraction prescription schemes. Materials and Methods We incorporated the Lea-Catcheside dose protraction factor g, the effective tumor doubling time Td, the total elapsed time of the treatment course T, and the onset or lag time of cell repopulation Tk, into the full-form BED calculation, in contrast to the simple form BED which only includes the total dose, dose per fraction and α/β. The Poisson model relating the surviving fraction and the number of tumor clonogens (K) was used to calculate TCP. The parameter set α = 0.15 Gy-1, α/β = 3.1 Gy, τ = 0.27 h (DNA damage repair half time), Td = 42 days, and Tk = 0 was used for the full-form BED calculation. K = 1.1 × 107 from the high-risk group was used in the TCP calculation. The new 192Ir source (40,700 U, 10 Ci, 1.27 Gy/min) and the 90-day source (17,470 U, 4.3 Ci, 0.55 Gy/min) were used to investigate the source decay effect on TCP. Three different fractionation schemes n = 1, 2, and 9 fraction(s) were studied. Simple BED, full-form BED (both 10 Ci and 4.3 Ci), TCP50 (total dose at TCP = 50%), and TCP90 (total dose at TCP = 90%) were calculated for each setup. 1 x 21 Gy, 2 x 13.5 Gy, and 9 x 6 Gy prescriptions were selected to evaluate the robustness of different fractionation schemes on TCP impacted by DNA damage repair and source decay. Results TCP50 and TCP90 using the simple BED, the full-form BED at 10 Ci and 4.3 Ci were calculated. In the single-fraction group, TCP50 = 17.0, 18.6, and 21.2 Gy, and TCP90 = 18.0, 19.9, and 22.8 Gy. In the 2-fraction group, TCP50 = 23.3, 24.7, and 26.8 Gy, and TCP90 = 24.7, 26.3, and 28.7 Gy. In the 9-fraction group, TCP50 = 43.3, 44.3, and 45.6 Gy, and TCP90 = 46.3, 47.4, and 48.9 Gy. For 1 × 21 Gy, the simple BED and full-form BED (10 Ci and 4.3 Ci) = 163.3, 134.8, and 109.0 Gy, and TCP = 99.9%, 98.2%, and 41.9%. For 2 × 13.5 Gy, the simple BED and full-from BED (10 Ci and 4.3 Ci) = 144.6, 128.5, and 112.0 Gy, and TCP = 99.6%, 95.4%, and 57.4%. For 9 × 6 Gy, the simple BED and full-from BED (10 Ci and 4.3 Ci) = 158.5, 151.4, and 143.4 Gy, and TCP = 99.9%, 99.9%, and 99.5%. In general, we have observed: (1) using the simple BED overestimated the TCP compared to the full-form BED, (2) with the source decay, a higher total dose was needed to achieve the same level of TCP, (3) using the hypo-fractionation saved total dose and total irradiation time to achieve the same TCP, but (4) using the hyper-fractionation can dampen the effects of DNA damage repair and source decay on TCP. Conclusions The changes in BED introduced by the Lea-Catcheside dose protraction factor into our TCP model were most significant for deliveries with a long treatment time and/or a decayed source. Current prescriptions for 1, 2, and 9 fraction(s) are adequate to reach TCP of at least 41.9%, 57.4%, and 99.5%. In the conventional fractionation schemes of high-dose-rate (HDR) brachytherapy, the intra-fractional and inter-fractional DNA damage repair and repopulation of tumor cells are neglected in calculating the biologically effective dose (BED). This may result in inaccurate model prediction of the theoretical tumor control probability (TCP). Notwithstanding, current prostate brachytherapy prescriptions may still be large enough to theoretically overcome these effects, among others. The purpose of this study was to recalculate the theoretical TCP, accounting for intrafraction DNA damage repair and 192Ir source decay for prostate cancer treated using HDR brachytherapy as the monotherapy, compared against common 1-, 2-, and 9-fraction prescription schemes. We incorporated the Lea-Catcheside dose protraction factor g, the effective tumor doubling time Td, the total elapsed time of the treatment course T, and the onset or lag time of cell repopulation Tk, into the full-form BED calculation, in contrast to the simple form BED which only includes the total dose, dose per fraction and α/β. The Poisson model relating the surviving fraction and the number of tumor clonogens (K) was used to calculate TCP. The parameter set α = 0.15 Gy-1, α/β = 3.1 Gy, τ = 0.27 h (DNA damage repair half time), Td = 42 days, and Tk = 0 was used for the full-form BED calculation. K = 1.1 × 107 from the high-risk group was used in the TCP calculation. The new 192Ir source (40,700 U, 10 Ci, 1.27 Gy/min) and the 90-day source (17,470 U, 4.3 Ci, 0.55 Gy/min) were used to investigate the source decay effect on TCP. Three different fractionation schemes n = 1, 2, and 9 fraction(s) were studied. Simple BED, full-form BED (both 10 Ci and 4.3 Ci), TCP50 (total dose at TCP = 50%), and TCP90 (total dose at TCP = 90%) were calculated for each setup. 1 x 21 Gy, 2 x 13.5 Gy, and 9 x 6 Gy prescriptions were selected to evaluate the robustness of different fractionation schemes on TCP impacted by DNA damage repair and source decay. TCP50 and TCP90 using the simple BED, the full-form BED at 10 Ci and 4.3 Ci were calculated. In the single-fraction group, TCP50 = 17.0, 18.6, and 21.2 Gy, and TCP90 = 18.0, 19.9, and 22.8 Gy. In the 2-fraction group, TCP50 = 23.3, 24.7, and 26.8 Gy, and TCP90 = 24.7, 26.3, and 28.7 Gy. In the 9-fraction group, TCP50 = 43.3, 44.3, and 45.6 Gy, and TCP90 = 46.3, 47.4, and 48.9 Gy. For 1 × 21 Gy, the simple BED and full-form BED (10 Ci and 4.3 Ci) = 163.3, 134.8, and 109.0 Gy, and TCP = 99.9%, 98.2%, and 41.9%. For 2 × 13.5 Gy, the simple BED and full-from BED (10 Ci and 4.3 Ci) = 144.6, 128.5, and 112.0 Gy, and TCP = 99.6%, 95.4%, and 57.4%. For 9 × 6 Gy, the simple BED and full-from BED (10 Ci and 4.3 Ci) = 158.5, 151.4, and 143.4 Gy, and TCP = 99.9%, 99.9%, and 99.5%. In general, we have observed: (1) using the simple BED overestimated the TCP compared to the full-form BED, (2) with the source decay, a higher total dose was needed to achieve the same level of TCP, (3) using the hypo-fractionation saved total dose and total irradiation time to achieve the same TCP, but (4) using the hyper-fractionation can dampen the effects of DNA damage repair and source decay on TCP. The changes in BED introduced by the Lea-Catcheside dose protraction factor into our TCP model were most significant for deliveries with a long treatment time and/or a decayed source. Current prescriptions for 1, 2, and 9 fraction(s) are adequate to reach TCP of at least 41.9%, 57.4%, and 99.5%.
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PO61
目的在传统的高剂量率(HDR)近距离放射治疗的分离方案中,在计算生物有效剂量(BED)时忽略了片段内和片段间DNA损伤修复和肿瘤细胞的再生。这可能导致理论肿瘤控制概率(TCP)的模型预测不准确。尽管如此,目前的前列腺近距离治疗处方可能仍然足够大,理论上可以克服这些影响。本研究的目的是重新计算理论TCP,将HDR近距离放疗作为单一疗法治疗前列腺癌时的DNA损伤修复和192Ir源衰减与常见的1-、2-和9-组分处方方案进行比较。材料与方法我们将lea - catch - side剂量延长因子g、肿瘤有效倍增时间Td、疗程总时间T、细胞再生开始或滞后时间Tk纳入全形式BED计算,而不是只包括总剂量、每组分剂量和α/β的简单形式BED计算。采用生存分数与肿瘤克隆原数(K)的泊松模型计算TCP。参数集α = 0.15 Gy-1, α/β = 3.1 Gy, τ = 0.27 h (DNA损伤修复一半时间),Td = 42天,Tk = 0进行全形态BED计算。TCP计算采用高危组K = 1.1 × 107。利用新的192Ir源(40,700 U, 10 Ci, 1.27 Gy/min)和90天源(17,470 U, 4.3 Ci, 0.55 Gy/min)研究了源衰减对TCP的影响。研究了三种不同的分馏方案n = 1、2和9个分数。分别计算简单BED、全形态BED (10 Ci和4.3 Ci)、TCP50 (TCP = 50%时的总剂量)和TCP90 (TCP = 90%时的总剂量)。选择1 x 21 Gy, 2 x 13.5 Gy和9 x 6 Gy处方来评估不同分离方案对DNA损伤修复和源衰变影响的TCP的稳健性。结果计算简单BED下的TCP50和TCP90,完整BED在10 Ci和4.3 Ci下的TCP90。在单段组中,TCP50 = 17.0、18.6和21.2 Gy, TCP90 = 18.0、19.9和22.8 Gy。在2-分数组中,TCP50 = 23.3、24.7和26.8 Gy, TCP90 = 24.7、26.3和28.7 Gy。在9个分数组中,TCP50 = 43.3、44.3和45.6 Gy, TCP90 = 46.3、47.4和48.9 Gy。对于1 × 21 Gy,简单BED和完整BED (10 Ci和4.3 Ci)分别为163.3、134.8和109.0 Gy, TCP分别为99.9%、98.2%和41.9%。对于2 × 13.5 Gy,简单BED和full-from BED (10 Ci和4.3 Ci)分别为144.6、128.5和112.0 Gy, TCP分别为99.6%、95.4%和57.4%。对于9 × 6 Gy,简单BED和full-from BED (10 Ci和4.3 Ci)分别为158.5、151.4和143.4 Gy, TCP分别为99.9%、99.9%和99.5%。总的来说,我们观察到:(1)与完整形式的BED相比,使用简单的BED高估了TCP;(2)与源衰变相比,需要更高的总剂量才能达到相同的TCP水平;(3)使用低分割可以节省总剂量和总照射时间以达到相同的TCP水平;(4)使用超分割可以抑制DNA损伤修复和源衰变对TCP的影响。在我们的TCP模型中,由lea - catchside剂量延长因子引入的BED变化在治疗时间较长和/或源衰变的分娩中最为显著。目前1、2和9分数的处方足以达到至少41.9%、57.4%和99.5%的TCP。在传统的高剂量率(HDR)近距离放射治疗的分离方案中,在计算生物有效剂量(BED)时忽略了片段内和片段间DNA损伤修复和肿瘤细胞的再生。这可能导致理论肿瘤控制概率(TCP)的模型预测不准确。尽管如此,目前的前列腺近距离治疗处方可能仍然足够大,理论上可以克服这些影响。本研究的目的是重新计算理论TCP,将HDR近距离放疗作为单一疗法治疗前列腺癌时的DNA损伤修复和192Ir源衰减与常见的1-、2-和9-组分处方方案进行比较。我们将lea - catch - side剂量延长因子g、有效肿瘤倍增时间Td、治疗过程总时间T和细胞再生开始或滞后时间Tk纳入完整形式的BED计算,而不是只包括总剂量、每组分剂量和α/β的简单形式BED。采用生存分数与肿瘤克隆原数(K)的泊松模型计算TCP。参数集α = 0.15 Gy-1, α/β = 3.1 Gy, τ = 0.27 h (DNA损伤修复一半时间),Td = 42天,Tk = 0进行全形态BED计算。TCP计算采用高危组K = 1.1 × 107。 目的在传统的高剂量率(HDR)近距离放射治疗的分离方案中,在计算生物有效剂量(BED)时忽略了片段内和片段间DNA损伤修复和肿瘤细胞的再生。这可能导致理论肿瘤控制概率(TCP)的模型预测不准确。尽管如此,目前的前列腺近距离治疗处方可能仍然足够大,理论上可以克服这些影响。本研究的目的是重新计算理论TCP,将HDR近距离放疗作为单一疗法治疗前列腺癌时的DNA损伤修复和192Ir源衰减与常见的1-、2-和9-组分处方方案进行比较。材料与方法我们将lea - catch - side剂量延长因子g、肿瘤有效倍增时间Td、疗程总时间T、细胞再生开始或滞后时间Tk纳入全形式BED计算,而不是只包括总剂量、每组分剂量和α/β的简单形式BED计算。采用生存分数与肿瘤克隆原数(K)的泊松模型计算TCP。参数集α = 0.15 Gy-1, α/β = 3.1 Gy, τ = 0.27 h (DNA损伤修复一半时间),Td = 42天,Tk = 0进行全形态BED计算。TCP计算采用高危组K = 1.1 × 107。利用新的192Ir源(40,700 U, 10 Ci, 1.27 Gy/min)和90天源(17,470 U, 4.3 Ci, 0.55 Gy/min)研究了源衰减对TCP的影响。研究了三种不同的分馏方案n = 1、2和9个分数。分别计算简单BED、全形态BED (10 Ci和4.3 Ci)、TCP50 (TCP = 50%时的总剂量)和TCP90 (TCP = 90%时的总剂量)。选择1 x 21 Gy, 2 x 13.5 Gy和9 x 6 Gy处方来评估不同分离方案对DNA损伤修复和源衰变影响的TCP的稳健性。结果计算简单BED下的TCP50和TCP90,完整BED在10 Ci和4.3 Ci下的TCP90。在单段组中,TCP50 = 17.0、18.6和21.2 Gy, TCP90 = 18.0、19.9和22.8 Gy。在2-分数组中,TCP50 = 23.3、24.7和26.8 Gy, TCP90 = 24.7、26.3和28.7 Gy。在9个分数组中,TCP50 = 43.3、44.3和45.6 Gy, TCP90 = 46.3、47.4和48.9 Gy。对于1 × 21 Gy,简单BED和完整BED (10 Ci和4.3 Ci)分别为163.3、134.8和109.0 Gy, TCP分别为99.9%、98.2%和41.9%。对于2 × 13.5 Gy,简单BED和full-from BED (10 Ci和4.3 Ci)分别为144.6、128.5和112.0 Gy, TCP分别为99.6%、95.4%和57.4%。对于9 × 6 Gy,简单BED和full-from BED (10 Ci和4.3 Ci)分别为158.5、151.4和143.4 Gy, TCP分别为99.9%、99.9%和99.5%。总的来说,我们观察到:(1)与完整形式的BED相比,使用简单的BED高估了TCP;(2)与源衰变相比,需要更高的总剂量才能达到相同的TCP水平;(3)使用低分割可以节省总剂量和总照射时间以达到相同的TCP水平;(4)使用超分割可以抑制DNA损伤修复和源衰变对TCP的影响。在我们的TCP模型中,由lea - catchside剂量延长因子引入的BED变化在治疗时间较长和/或源衰变的分娩中最为显著。目前1、2和9分数的处方足以达到至少41.9%、57.4%和99.5%的TCP。在传统的高剂量率(HDR)近距离放射治疗的分离方案中,在计算生物有效剂量(BED)时忽略了片段内和片段间DNA损伤修复和肿瘤细胞的再生。这可能导致理论肿瘤控制概率(TCP)的模型预测不准确。尽管如此,目前的前列腺近距离治疗处方可能仍然足够大,理论上可以克服这些影响。本研究的目的是重新计算理论TCP,将HDR近距离放疗作为单一疗法治疗前列腺癌时的DNA损伤修复和192Ir源衰减与常见的1-、2-和9-组分处方方案进行比较。我们将lea - catch - side剂量延长因子g、有效肿瘤倍增时间Td、治疗过程总时间T和细胞再生开始或滞后时间Tk纳入完整形式的BED计算,而不是只包括总剂量、每组分剂量和α/β的简单形式BED。采用生存分数与肿瘤克隆原数(K)的泊松模型计算TCP。参数集α = 0.15 Gy-1, α/β = 3.1 Gy, τ = 0.27 h (DNA损伤修复一半时间),Td = 42天,Tk = 0进行全形态BED计算。TCP计算采用高危组K = 1.1 × 107。 利用新的192Ir源(40,700 U, 10 Ci, 1.27 Gy/min)和90天源(17,470 U, 4.3 Ci, 0.55 Gy/min)研究了源衰减对TCP的影响。研究了三种不同的分馏方案n = 1、2和9个分数。分别计算简单BED、全形态BED (10 Ci和4.3 Ci)、TCP50 (TCP = 50%时的总剂量)和TCP90 (TCP = 90%时的总剂量)。选择1 x 21 Gy, 2 x 13.5 Gy和9 x 6 Gy处方来评估不同分离方案对DNA损伤修复和源衰变影响的TCP的稳健性。TCP50和TCP90使用简单BED,在10 Ci和4.3 Ci下计算完整形式的BED。在单段组中,TCP50 = 17.0、18.6和21.2 Gy, TCP90 = 18.0、19.9和22.8 Gy。在2-分数组中,TCP50 = 23.3、24.7和26.8 Gy, TCP90 = 24.7、26.3和28.7 Gy。在9个分数组中,TCP50 = 43.3、44.3和45.6 Gy, TCP90 = 46.3、47.4和48.9 Gy。对于1 × 21 Gy,简单BED和完整BED (10 Ci和4.3 Ci)分别为163.3、134.8和109.0 Gy, TCP分别为99.9%、98.2%和41.9%。对于2 × 13.5 Gy,简单BED和full-from BED (10 Ci和4.3 Ci)分别为144.6、128.5和112.0 Gy, TCP分别为99.6%、95.4%和57.4%。对于9 × 6 Gy,简单BED和full-from BED (10 Ci和4.3 Ci)分别为158.5、151.4和143.4 Gy, TCP分别为99.9%、99.9%和99.5%。总的来说,我们观察到:(1)与完整形式的BED相比,使用简单的BED高估了TCP;(2)与源衰变相比,需要更高的总剂量才能达到相同的TCP水平;(3)使用低分割可以节省总剂量和总照射时间以达到相同的TCP水平;(4)使用超分割可以抑制DNA损伤修复和源衰变对TCP的影响。在我们的TCP模型中,由lea - catchside剂量延长因子引入的BED变化对于治疗时间较长和/或源衰变的分娩最为显著。目前1、2和9分数的处方足以达到至少41.9%、57.4%和99.5%的TCP。
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