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电离势

电离势的相关文献在1956年到2021年内共计122篇,主要集中在化学、物理学、无线电电子学、电信技术 等领域,其中期刊论文117篇、会议论文5篇、专利文献15870篇;相关期刊65种,包括滨州学院学报、衡阳师范学院学报、烟台大学学报(自然科学与工程版)等; 相关会议5种,包括第十一届全国应用化学年会、第十届全国原子与分子物理学术会议、中国化学会2000年学术会议等;电离势的相关文献由272位作者贡献,包括姜明、朱正和、盛六四等。

电离势—发文量

期刊论文>

论文:117 占比:0.73%

会议论文>

论文:5 占比:0.03%

专利文献>

论文:15870 占比:99.24%

总计:15992篇

电离势—发文趋势图

电离势

-研究学者

  • 姜明
  • 朱正和
  • 盛六四
  • 程新路
  • 英柏宁
  • 李文佐
  • 武国华
  • 裴玲
  • 唐永建
  • 宫宝安
  • 期刊论文
  • 会议论文
  • 专利文献

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    • 张晓琳; 焉炳飞; 刘绍丽; 李文佐
    • 摘要: 应用B3LYP方法和6-311G(d,p)、6-311++G(d,p)、cc-pVTZ基组对全部(共6种)氯代乙烯阳离子进行了理论研究,优化了它们的电子基态的结构,计算了各自对应分子的垂直电离势(VIP)和绝热电离势(AIP).结果表明,与具有非平面结构的乙烯阳离子不同,六种氯代乙烯阳离子均为平面构型.与分子结构相比,离子的C—Cl键缩短,C=C键增长.计算的各个分子的VIP和AIP与实验值符合的很好.
    • 王亚超; 林晓然; 王梅; 王吉芳; 陈玲
    • 摘要: 短-中链饱和甘油三酯是一种黏度低、可降解的液体绝缘材料,在变压器内绝缘领域具有潜在的应用价值.本文通过设置与绝缘油中放电相当的电场强度等级,使用密度泛函与含时密度泛函方法研究了短-中链饱和甘油三酯分子在电场影响下的分子特性变化规律.研究结果表明,电场下分子结构发生明显改变,分子键长与电场存在明显的依赖关系;相同电场下,随着碳链长度的增大,分子的偶极矩增大,分子极性增强;在109 V/m量级的电场强度下,三辛酸甘油酯与三癸酸甘油酯的最高占据态分子轨道能量明显增大,电离势急剧减小;分子间的激发特性差异较小,都随着电场强度的增大呈现出减小趋势,且相同电场下分子激发能的减小幅度远小于电离势的减小幅度.研究结果有助于提高人们对酯类绝缘介质中放电机理的认识,并为天然酯绝缘油的性能改进提供一定的理论支撑.
    • 裴玲; 李峰
    • 摘要: 本文采用量子化学的密度泛函理论(DFT)方法,从静态与动态两大方面分析了亚胺白藜芦醇不同位置酚羟基在不同溶剂中抗氧化活性的能力大小.从前线分子轨道初步分析了其抗氧化活性位点,通过对化合物酚羟基键解离焓(BDE)、电离势(IP)、质子解离焓(PDE)、质子亲和势(PA)和电子转移焓(ETE)等参数的研究,分析了一步抽氢反应机制(HAT)、逐步质子转移-电子转移机制(SET-PT)、质子优先损失电子转移机制(SPLET)三种反应机制,进一步确定了亚胺白藜芦醇的抗氧化活性位点.探讨了亚胺白藜芦醇分子不同位置酚羟基清除·OH和·OOH的抗氧化机理,得到了该分子与·OH和·OOH发生抽氢反应时的过渡态结构.计算结果表明,在溶剂中亚胺白藜芦醇分子C4'位上酚羟基活性最高,发生抽氢反应时所需能垒最小,是最大可能的活性位点.在非极性溶剂中HAT是主要的机制;在极性溶剂中SPLET机制是主要的.
    • 邢伟; 孙金锋; 施德恒; 朱遵略
    • 摘要: In this paper, we study the spectroscopic properties and predissociation mechanisms of 14 states, which come from the first two dissociation channels of the BF+ cation. The potential energy curves of 14 Λ-S (X2Σ+, 12Π, 22Π, 22Σ+,14Σ+, 14Δ, 14Σ-, 12Δ, 12Σ-, 32Σ+, 14Π, 24Π, 24Σ+, and 32Π) and corresponding 30 Ω states are calculated using the complete active space self-consistent field method, which is followed by the valence internally contracted multireference configuration interaction approach with the Davidson modification. To improve the reliability and accuracy of the potential energy curves, the core-valence correlation and scalar relativistic corrections, as well as the extrapolation of potential energy to the complete basis set limit are taken into account. The spin-orbit coupling is computed using the state interaction approach with the Breit-Pauli Hamiltonian. Based on these potential energy curves, the spectroscopic parameters and vibrational levels are determined for all the bound and quasi-bound Λ-S and Ω states. The present ground-state spectroscopic constants match well with the available experimental data. In addition, the vertical and adiabatic ionization potentials from the X1Σ+ state of BF molecule to the X2Σ+, 12Π, and 22Σ+ states of BF+ cation are calculated. The results of BF+(X2Σ+)←BF(X1Σ+) ionization are in good agreement with the measurements. Various curve crossings of Λ-S states are revealed. We calculate the spin-orbit matrix elements between two interacting electronic states in the curve crossing region. With the help of present spin-orbit coupling matrix elements, we analyze the predissociation mechanisms of X2Σ+ and 32Π states along with the perturbations of the nearby states to 22Π, 14Σ+ and 32Σ+ states for the first time. The predissociation of X2Σ+ and 32Π states have a chance to occur around the vibrational levels υ"= 30 and υ'= 0 due to spin-orbit coupling, respectively. The present results also indicate that the υ' ≥ 9 vibrational levels of 22Π state are perturbed by the crossing states 22Σ+, 14Σ+, 14Δ, 14Σ-, 12Δ, 12Σ-, 32Σ+,and 14Π, that the υ' ≥ 4 vibrational levels of 14Σ+ state are perturbed via the interacting states 14Π- and 12Π-, and the great perturbations between υ' ≥ 4 vibrational levels of 32Σ+ state and υ' ≥ 0 vibrational levels of 14Π state. For the 30Ω state, we also calculate the relative energies of dissociation limits compared with the lowest one matching well with the experimental ones. Finally, the Franck-Condon factors, Einstein coefficients, and radiative lifetimes are evaluated for the 22Π (υ'= 0–9)–X2Σ+, 22Σ+ (υ'= 0–2)–X2Σ+, (3)1/2–(1)1/21st well, and (2)3/2 (υ'= 0–9)–(1)1/21st well transitions.%采用考虑Davidson修正的内收缩多参考组态相互作用(icMRCI+Q)方法,结合相关一致基组aug-cc-pV5Z和aug-cc-pV6Z,计算了BF+离子前两个离解极限B+(1Sg)+F(2Pu)和B+(3Pu)+F(2Pu)对应的14个Λ-S态(X2Σ+,12Π,22Π,22Σ+,14Σ+,14?,14Σ-,12?,12Σ-,32Σ+,14Π,24Π,24Σ+和32Π)和30个?态的势能曲线.在势能曲线的计算中,考虑了旋轨耦合效应、核价相关和标量相对论修正以及将参考能和相关能分别外推至完全基组极限.基于得到的势能曲线,获得了束缚和准束缚的12个Λ-S态和28个?态的光谱常数,并且X2Σ+态的光谱常数与已有的实验结果符合.此外,计算了BF分子X1Σ+态到BF+离子X2Σ+,12Π和22Σ+态的垂直电离势和绝热电离势,并且BF+(X2Σ+)←BF(X1Σ+)的垂直电离势和绝热电离势与相应的实验结果非常符合.由X2Σ+,22Π,14Σ+,32Σ+和32Π态和其他的激发Λ-S态势能曲线的交叉现象,借助于计算的旋轨耦合矩阵元,首次分析了X2Σ+和32Π态的预解离机理以及22Π(υ′>9),14Σ+(υ′>4)和32Σ+(υ′>4)的振动能级受到其他电子态的微扰.计算了30个?态离解极限处的相对能量,并且与实验结果十分符合.最后计算了22Π(υ′=0-9)-X2Σ+,22Σ+(υ′=0-2)-X2Σ+,(3)1/2-(1)1/2势阱一和(2)3/2(υ′=0-9)-(1)1/2势阱一跃迁的Franck-Condon因子、爱因斯坦自发辐射系数和辐射寿命.
    • 董志敏; 徐培波; 张颜辉; 史相强; 柳兆良; 郭丽华; 李连鑫; 杨晓勇
    • 摘要: 从理论上考察了一种新型超卤素阴离子体系MX-3(M=Be,Mg,Ca;X=F,Cl,Br),并对该体系的几何结构、成键特征等性质进行了详细研究.上述MX-3的全实频率的几何优化结构在MP2/6-311+G(d)水平下得到并进行自然键轨道(NBO)分析,证实所有的MX-3均具有平面几何结构.所研究的MX-3表现出相当大的HOMO-LUMO能隙值,说明它们具有很好的稳定性.这些MX-3的电离势IP值均高于Cl原子的电子亲和势EA值,因此可以视其为超卤素阴离子.量子化学计算结果表明MX-3体系中卤素配体的原子尺寸可以影响其电离势值:配体尺寸越小,电离势值越低.
    • 董志敏; 徐培波; 张颜辉; 史相强; 柳兆良; 郭丽华; 李连鑫; 杨晓勇
    • 摘要: 从理论上考察了一种新型超卤素阴离子体系MX3-(M=Be,Mg,Ca; X=F,Cl,Br),并对该体系的几何结构、成键特征等性质进行了详细研究。上述MX3-的全实频率的几何优化结构在MP2/6-311+G(d)水平下得到并进行自然键轨道(NBO)分析,证实所有的MX3-均具有平面几何结构。所研究的MX3-表现出相当大的HOMO-LUMO能隙值,说明它们具有很好的稳定性。这些MX3-的电离势IP值均高于Cl原子的电子亲和势EA值,因此可以视其为超卤素阴离子。量子化学计算结果表明MX3-体系中卤素配体的原子尺寸可以影响其电离势值:配体尺寸越小,电离势值越低。
    • 董志敏1; 徐培波1; 张颜辉1; 史相强1; 柳兆良1; 郭丽华1; 李连鑫1; 杨晓勇1
    • 摘要: 从理论上考察了一种新型超卤素阴离子体系MX3^-(M=Be,Mg,Ca;X=F,Cl,Br),并对该体系的几何结构、成键特征等性质进行了详细研究。上述MX3^-的全实频率的几何优化结构在MP2/6-311+G(d)水平下得到并进行自然键轨道(NBO)分析,证实所有的MX3^-均具有平面几何结构。所研究的MX3^-表现出相当大的HOMOLUMO能隙值,说明它们具有很好的稳定性。这些MX3^-的电离势IP值均高于Cl原子的电子亲和势EA值,因此可以视其为超卤素阴离子。量子化学计算结果表明MX3^-体系中卤素配体的原子尺寸可以影响其电离势值:配体尺寸越小,电离势值越低。
    • 裴玲; 徐秋红
    • 摘要: Based on the structure of resveratrol (A),six resveratrol analogues (B-G) were designed.Then the relationship between the structure and antioxidant activity of resveratrol and its derivatives were studied in the gas phase and solvents using quantum chemical calculations based on the density functional theory (DFT).The three main working mechanisms,H-atom transfer (HAT),single electron transfer-proton transfer (SET-PT) and sequential proton loss electron transfer (SPLET) were investigated.The result showed that HAT would be the most favorable mechanism for explaining the radical-scavenging activity of four compounds in the gas phase,whereas the SPLET mechanism would be the thermodynamically favorable pathway in polar solvents.The calculations suggested that,SET-PT was not the most preferred mechanism in all environments studied.%本研究在白藜芦醇(A)结构的基础上设计了6种白藜芦醇类似物(B-G),采用量子化学密度泛函理论(DFT)计算方法,在气相和溶剂中研究了白藜芦醇及其6种类似物的结构与抗氧化活性的关系.对三种抗氧化机制:抽氢反应(HAT)机制、逐步电子转移质子转移(SET-PT)机制、质子优先损失电子转移(SPLET)机制进行了研究.计算结果表明,在气相中抽氢反应机制是化合物清除自由基活性的最主要机制,在极性溶剂中SPLET机制是热力学上最有利的途径,而在所有环境中SET-PT机制都不是最主要的机制.
    • 裴玲; 卞贺
    • 摘要: 采用量子化学密度泛函理论(DFT)计算方法,在B3LYP/6-311G(d,p)水平下对白藜芦醇及其衍生物(a-h)进行了优化,在优化构型的基础上采用B3LYP/6-311++G(2d,2p)进行了单点能计算.通过该类化合物酚羟基键解离焓(BDE)、电离势(IP)、质子解离焓(PDE)、质子亲和势(PA)和电子转移焓(ETE)等参数对9种物质的抗氧化机理(抽氢反应机理、逐步电子转移质子转移和质子优先损失电子转移机理)进行了研究.结果表明,不同位置酚羟基的活性不同,B环C4’位酚羟基的活性最强.对于不同的抗氧化机理,不同的物质表现出了不同的抗氧化活性,抽氢反应机理表明各物质的抗氧化性顺序为Res >e >a >b≈d≈g>f≈h >e,逐步电子转移质子转移机理表明各物质的抗氧化性Res>e>h≈a>f>d>b>g>c,质子优先损失电子转移机理表明各物质的抗氧化性顺序为d>Res>e>f>h>a>b>g>c.
    • 邢伟; 刘慧; 施德恒; 孙金锋; 朱遵略
    • 摘要: 采用考虑Davidson修正的内收缩多参考组态相互作用(icMRCI+Q)方法结合相关一致基组aug-cc-pV5Z和aug-cc-pV6Z计算了CF+离子第一离解极限C+(2Pu)+F(2Pu)对应的12个Λ-S态(X1Σ+, a3Π,13Σ+,13∆,11∆,11Σ−,13Σ−,21Σ+,11Π,23Π,21Π和23Σ+)所产生的23个Ω态的势能曲线。计算中考虑了旋轨耦合效应、核价相关和标量相对论修正以及将参考能和相关能分别外推至完全基组极限。基于得到的势能曲线,获得了束缚和准束缚的9个Λ-S态和16个Ω态的光谱常数,并且X1Σ+, a3Π势阱一Λ-S态的光谱常数与已有的实验结果非常符合。此外,计算了CF自由基X2Π态到CF+离子束缚和准束缚的9个Λ-S态的垂直电离势和绝热电离势,并且CF+(X1Σ+)←CF(X2Π)和CF+(a3Π势阱一)←CF(X2Π)的垂直电离势和绝热电离势与相应的实验结果也非常符合。由a3Π,11Π态和其他激发Λ-S态势能曲线的交叉现象,借助于计算的旋轨耦合矩阵元,分析了a3Π势阱一,11Π势阱一和21Σ+态的预解离机理。计算的23个Ω态离解极限处的相对能量与实验结果十分吻合。最后计算了(2)0+势阱一(υ′=0—5),(1)1势阱一(υ′=0—5)和(2)1势阱一(υ′=0)到X0+态跃迁的Franck-Condon因子和辐射寿命。%The potential energy curves of twenty-threeΩstates generated from the twelveΛ-S states (X1Σ+, a3Π, 13Σ+, 13∆, 11∆, 11Σ−, 13Σ−, 21Σ+, 11Π, 23Π, 21Π and 23Σ+) correlating with the first dissociation channel C+ (2Pu)+ F(2Pu) of the CF+ cation are obtained by using the internally contracted multireference configuration interaction approach with the Davidson modification (icMRCI+Q) on the basis of the correlation-consistent aug-cc-pV5Z and aug-cc-pV6Z basis sets for the first time. The spin-orbit coupling, core-valence correlation and relativistic corrections are taken into account, and all the potential energy curves are extrapolated to the complete basis set limit by separately extrapolating the Hartree-Fock and correlation energies scheme. Based on the calculated potential energy curves, the spectroscopic parameters of the bound and quasibound nine Λ-S and sixteen Ω states of the CF+ cation are obtained. And the spectroscopic parameters of X1Σ+and a3Π1st well Λ-S states which are in very good agreement with experimental results are achieved. Furthermore, the vertical and adiabatic ionization potentials of ionization from the X2Πstate of CF radical to the bound and quasibound nineΛ-S states of the CF+ cation are calculated, and the vertical and adiabatic ionization potentials of the CF+(X1Σ+) ←CF(X2Π) and CF+(a3Π1st well) ←CF(X2Π) ionizations are also in good agreement with the corresponding experimental values. Various curve crossings of Λ-S states are revealed, and with the help of our computed spin-orbit coupling matrix elements, the predissociation mechanisms of the a3Π1st well, 11Π1st well and 21Σ+ states are analyzed for the first time. The spin-orbit-induced predissociations for the a3Π1st well, 11Π1st well and 21Σ+Λ-S states could happen, and the predissociations of the a3Π1st well, 11Π1st well and 21Σ+Λ-S states start around the vibrational levels υ′ = 15, υ′ = 1 and υ′ = 1, respectively. Relative energies of the twenty-three Ω states in the dissociation limits are given, and our calculations match the experimental results very well. Finally, the Franck-Condon factors and radiative lifetimes of transitions from (2) 0+ 1st well (υ′=0–5), (1) 11st well (υ′=0–5) and (2) 11st well (υ′=0) to X0+Ωstates are predicted for the future laboratory research.
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