Anil Kumar*, Michael D. Sevilla* and Leon Sanche*,
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We considered the nucleotide with the G–C base pair (ds[5′-G-3′]) as a model for electron localization in the DNA double helix and calculated the potential energy surfaces (PESs) of excited states of the ground-state TA of ds[5′-G-3′], which correspond to shape and core-excited resonances. The calculations show that shape TAs start at ca. 1 eV, while core-excited TAs occur only above 4 eV. The energy profile of each excited state and the corresponding PES are obtained by simultaneously stretching both C5′–O5′ bonds of ds[5′-G-3′]. From the nature of the PES, we find two dissociative (σ*) states localized on the PO<sub>4</sub> groups at the C5′ sites of ds[5′-G-3′]. The first σ* state at 1 eV is due to a shape resonance, while the second σ* state is induced by a core-excited resonance at 5.4 eV. As the bond of the latter state stretches and arrives close to the dissociation limit, the added electron on C transfers to C5′ phosphate, thus demonstrating the possibility of producing a DSB with only one electron of ca. 5 eV.</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":"128 17","pages":"4053–4062"},"PeriodicalIF":2.8000,"publicationDate":"2024-04-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.acs.org/doi/epdf/10.1021/acs.jpcb.3c08367","citationCount":"0","resultStr":"{\"title\":\"How a Single 5 eV Electron Can Induce Double-Strand Breaks in DNA: A Time-Dependent Density Functional Theory Study\",\"authors\":\"Anil Kumar*, Michael D. 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We considered the nucleotide with the G–C base pair (ds[5′-G-3′]) as a model for electron localization in the DNA double helix and calculated the potential energy surfaces (PESs) of excited states of the ground-state TA of ds[5′-G-3′], which correspond to shape and core-excited resonances. The calculations show that shape TAs start at ca. 1 eV, while core-excited TAs occur only above 4 eV. The energy profile of each excited state and the corresponding PES are obtained by simultaneously stretching both C5′–O5′ bonds of ds[5′-G-3′]. From the nature of the PES, we find two dissociative (σ*) states localized on the PO<sub>4</sub> groups at the C5′ sites of ds[5′-G-3′]. The first σ* state at 1 eV is due to a shape resonance, while the second σ* state is induced by a core-excited resonance at 5.4 eV. 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引用次数: 0
摘要
低能(<20 eV)电子(LEEs)可与 DNA 发生共振作用,形成基本单元的瞬态阴离子(TAs),诱发单链断裂(SSBs)和双链断裂(DSBs)等群集损伤。形状共振产生于先前未填充轨道上的电子俘获,只能诱发 SSB,而实验证明单核激发共振(即空穴场激发轨道上的两个电子)可导致簇损伤。在此,我们通过时间相关密度泛函理论(TDDFT)证明,核激发共振可产生 DSB,即一个 5 eV 电子可在 DNA 中诱发两个相近的病变。我们将带有 G-C 碱基对(ds[5′-G-3′])的核苷酸视为 DNA 双螺旋中电子定位的模型,并计算了ds[5′-G-3′]基态 TA 激发态的势能面(PESs),它们分别对应于形状共振和核激发共振。计算结果表明,形状 TA 从大约 1 eV 开始,而核激发共振则从大约 1 eV 开始。1 eV,而核激发 TA 只发生在 4 eV 以上。通过同时拉伸ds[5′-G-3′] 的两个 C5′-O5′键,可以得到每个激发态的能谱和相应的 PES。从 PES 的性质来看,我们发现在 ds[5′-G-3′] C5′ 位点的 PO4 基团上存在两种离解(σ*)态。位于 1 eV 的第一个 σ* 态是由形状共振引起的,而第二个 σ* 态则是由位于 5.4 eV 的核激发共振引起的。当后一状态的键拉伸并接近解离极限时,C 上的附加电子转移到 C5′ 磷酸上,从而证明了只用一个约 5 eV 的电子产生 DSB 的可能性。
How a Single 5 eV Electron Can Induce Double-Strand Breaks in DNA: A Time-Dependent Density Functional Theory Study
Low-energy (<20 eV) electrons (LEEs) can resonantly interact with DNA to form transient anions (TAs) of fundamental units, inducing single-strand breaks (SSBs), and cluster damage, such as double-strand breaks (DSBs). Shape resonances, which arise from electron capture in a previously unfilled orbital, can induce only a SSB, whereas a single core-excited resonance (i.e., two electrons in excited orbitals of the field of a hole) has been shown experimentally to cause cluster lesions. Herein, we show from time-dependent density functional theory (TDDFT) that a core-excited resonance can produce a DSB, i.e., a single 5 eV electron can induce two close lesions in DNA. We considered the nucleotide with the G–C base pair (ds[5′-G-3′]) as a model for electron localization in the DNA double helix and calculated the potential energy surfaces (PESs) of excited states of the ground-state TA of ds[5′-G-3′], which correspond to shape and core-excited resonances. The calculations show that shape TAs start at ca. 1 eV, while core-excited TAs occur only above 4 eV. The energy profile of each excited state and the corresponding PES are obtained by simultaneously stretching both C5′–O5′ bonds of ds[5′-G-3′]. From the nature of the PES, we find two dissociative (σ*) states localized on the PO4 groups at the C5′ sites of ds[5′-G-3′]. The first σ* state at 1 eV is due to a shape resonance, while the second σ* state is induced by a core-excited resonance at 5.4 eV. As the bond of the latter state stretches and arrives close to the dissociation limit, the added electron on C transfers to C5′ phosphate, thus demonstrating the possibility of producing a DSB with only one electron of ca. 5 eV.
期刊介绍:
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