双核苷酸双链断裂是放射治疗的关键效应因子

Anders Brahme, Yvonne Lorat
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引用次数: 1

摘要

大多数电离辐射会产生≈1 keV 的 δ 射线,可对 100 nm3 体积的 DNA 产生 MGy 剂量。这些事件可在核小体上产生严重的双链断裂(DDSB),尤其是在密集的异染色质 DNA 中。这是最常见的多重损伤部位,其发生概率决定了不同类型辐射的生物有效性。我们将讨论它们的频率、对细胞存活的影响、DNA 修复以及金纳米粒子示踪剂和电子显微镜成像。这种新的、有价值的纳米分辨率信息可用于确定最佳的肿瘤治疗方法,最大限度地提高对肿瘤的治疗效果,同时最大限度地降低对正常组织的治疗效果。DDSBs 的产生使得向肿瘤提供相当高的剂量和 LET(>2.5 Gy/Fr),同时在 TP53 完整的受威胁正常组织中达到每部分约 1.8-2.3 Gy 的最低 LET 变得非常重要。因此,利用了其内在的低剂量高敏感性(LDHS)相关的最佳日分馏窗口。在 p53 完全激活 NHEJ 和 HR 修复(≈½ Gy)之前,低剂量凋亡(LDA)和 LDHS 可将正常组织的突变概率降至最低。因此,离子疗法最好能在正常组织中产生尽可能低的 LET,以避免 DDSB 的升高。氦到硼离子可以通过更高的 LET 布拉格峰来实现这一目标,从而增加肿瘤的 DDSB 密度。有趣的是,使用硼或更重的离子实现无并发症治愈的可能性最大,这需要在最后 10-15 GyE 采用低 LET 循环,从而使剂量反应陡峭化,进一步将正常组织损伤降至最低。总之,新的高分辨率 DSB 和 DDSB 诊断方法与新的更精确的基于 DNA 修复的放射生物学相结合,加深了我们对治疗性放射治疗的临床重要性的理解。事实上,我们必须明白,我们已经越过了最佳 LET 区域,需要后退一步,而不是向前迈进,目前正在考虑使用氧气。从远端肿瘤的高杀伤力和严重的高LET以及正常组织的LET增加(让人联想到中子或氖离子)可以看出,因此最好使用锂硼离子或将碳与最佳的10-15 GyE光子、电子或甚至质子辐照结合起来,从而实现优化的分次、根治性、近乎复杂的放射治疗、这样就可以利用光子、电子和光离子进行优化的、分次的、治疗性的、几乎无并发症的治疗,为治疗性放射治疗带来真正的范式转变,有可能提高肿瘤治疗效果 5 GyE,将无并发症治愈率提高 25%,并实现凋亡-衰减-布拉格峰分子光离子放射治疗。
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Dual Nucleosomal Double-Strand Breaks Are the Key Effectors of Curative Radiation Therapy
Most ionizing radiation produces δ-rays of ≈1 keV that can impart MGy doses to 100 nm3 volumes of DNA. These events can produce severe dual double-strand breaks (DDSBs) on nucleosomes, particularly in dense heterochromatic DNA. This is the most common multiply damaged site, and their probabilities determine the biological effectiveness of different types of radiation. We discuss their frequency, effect on cell survival, DNA repair, and imaging by gold nanoparticle tracers and electron microscopy. This new and valuable nanometer resolution information can be used for determining the optimal tumor cure by maximizing therapeutic effects on tumors and minimizing therapeutic effects on normal tissues. The production of DDSBs makes it important to deliver a rather high dose and LET to the tumor (>2.5 Gy/Fr) and at the same time reach approximately 1.8–2.3 Gy of the lowest possible LET per fraction in TP53 intact normal tissues at risk. Therefore, their intrinsic low-dose hyper-sensitivity (LDHS)-related optimal daily fractionation window is utilized. Before full p53 activation of NHEJ and HR repair at ≈½ Gy, the low-dose apoptosis (LDA) and LDHS minimize normal tissue mutation probabilities. Ion therapy should thus ideally produce the lowest possible LET in normal tissues to avoid elevated DDSBs. Helium to boron ions can achieve this with higher-LET Bragg peaks, producing increased tumor DDSB densities. Interestingly, the highest probability of complication-free cure with boron or heavier ions requires a low LET round-up for the last 10–15 GyE, thereby steepening the dose response and further minimizing normal tissue damage. In conclusion, the new high-resolution DSB and DDSB diagnostic methods, and the new more accurate DNA-repair-based radiation biology, have been combined to increase our understanding of what is clinically important in curative radiation therapy. In fact, we must understand that we already passed the region of optimal LET and need to go back one step rather than forward, with oxygen being contemplated. As seen by the high overkill and severely high LET in the distal tumor and the increased LET to normal tissues (reminding of neutrons or neon ions), it is therefore preferable to use lithium–boron ions or combine carbon with an optimal 10–15 GyE photon, electron, or perhaps even a proton round-up, thus allowing optimized, fractionated, curative, almost complication-free treatments with photons, electrons, and light ions, introducing a real paradigm shift in curative radiation therapy with a potential 5 GyE tumor boost, 25% increase in complication-free cure and apoptotic–senescent Bragg Peak molecular light ion radiation therapy.
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