用STM进行单分子反应的作用光谱——我个人从2001年开始的观点

IF 8.7 2区 工程技术 Q1 CHEMISTRY, PHYSICAL Progress in Surface Science Pub Date : 2018-12-01 DOI:10.1016/j.progsurf.2018.09.001
H. Ueba
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This enabled me to propose a formula for a reaction rate </span></span><span><math><mrow><mi>R</mi><mo>(</mo><mi>V</mi><mo>)</mo></mrow></math></span> or yield per electron <span><math><mrow><mi>Y</mi><mo>(</mo><mi>V</mi><mo>)</mo><mo>=</mo><mi>R</mi><mo>(</mo><mi>V</mi><mo>)</mo><mo>/</mo><mi>I</mi></mrow></math></span>, here <em>I</em> is a tunneling current, <em>i.e.,</em> action spectrum (STM-AS) of a single molecule reaction. I applied this formula to reproduce the experimental result of a CO molecule hopping on Pd (1<!--> <!-->1<!--> <!-->0) surface and more insights into the elementary process were revealed. Thomas Frederiksen and Magus Paulsson jointed me to develop a general formula of <span><math><mrow><mi>Y</mi><mo>(</mo><mi>V</mi><mo>)</mo></mrow></math></span> and successfully applied it to analyse the experimental results of H-atom relay reaction of a linear chain, H(D)<sub>2</sub>O-OH(D)-O(D) H → H(D)-H(D)<sub>2</sub>-OH(D)  → H(D)-H(D)-OH(D)<sub>2</sub><span> that was observed by Takashi Kumagai and Hiroshi Okuyama. Actually a hydrogen atom excited at one end of a linear chain composed of H</span><sub>2</sub>O and several OH generates another one at the other end. We employed our formula of to reproduce the experimental result of <span><math><mrow><mi>Y</mi><mo>(</mo><mi>V</mi><mo>)</mo></mrow></math></span>. It was found that excitation of the three characteristic vibrational modes (free OH/OD stretch, OH<sup>∗</sup> = OD<sup>∗</sup> stretch, and H<sub>2</sub>O scissors, where H<sup>∗</sup> = D<sup>∗</sup> denotes the shared H/D<sup>∗</sup> atom in the H bond) were involved in the relay reaction. It was remarked that the OH(D<sup>∗</sup>) = OD(D<sup>∗</sup><span><span> stretch modes are significantly redshifted from free OH/OD stretch and also characterized by very large broadening. The significant mode softening with respect to the free stretch modes and spectacular enhancement of the width are known to originate in the strong anharmonic character of a single H bond. Thomas investigated the reaction pathway from total energy calculations for the H-atom transfer reaction by the nudged elastic band method. The initial step is translation of the shared H-atom to the center </span>hydroxyl, which is almost barrierless. The subsequent H-bond cleavage between OH and the center water molecule constitutes the highest barrier in which the displacement of the center water molecule along the [0</span> <!-->0<!--> <!-->1] direction is mainly involved. The OH, OH<sup>∗</sup> stretch and H<sub>2</sub>O scissors modes are therefore postulated to couple to the reaction coordinate for the H-bond cleavage. We have demonstrated a vibrationally induced H-atom-bond relay reaction within H-bonded chains assembled on Cu(1<!--> <!-->1<!--> <!-->0). In this reaction H-atom transfer results in the ‘structural’ transfer of a water molecule from one end of the chain to the other end without changing the platform of the chain, or actually transferring the molecule.</p><p>I have been thinking the unresolved issue of C<sub>2</sub>H(D)<sub>2</sub> rotation on Cu (1<!--> <!-->0<!--> <!-->0) since it was published in 1998 by the W. Ho group. This experimental methods and the results obtained as the first demonstration of a single molecule switch are widely recognized as a milestone report of a single molecule manipulation by tunneling current and applied bias voltage which excites the vibrational modes of a molecule. They observed the STM images rotated at 90 degrees before and after applying appropriate bias voltage. They further compared the IETS spectrum and the <span><math><mrow><mi>Y</mi><mo>(</mo><mi>V</mi><mo>)</mo></mrow></math></span> for the rotation. The observed peak beautifully agreed with the threshold bias voltage, which clearly evidenced that a rotation is induced by excitation of a particular vibrational mode of C<sub>2</sub>H(D)<sub>2</sub>. In particular a crossover from a single electron process to a two electron process with increase in a tunneling current are of great interest. Sergei and his PhD student Yulia E. Shchadilova at that time and Magnus helped me much to reproduce all the experimental results by employing the Keldysh Green’s function theory combined with <em>ab initio</em><span> density functional theory (DFT) calculation of the optimized adsorption geometry and sophisticated vibrational analysis done by Magus. The experimental result of </span><span><math><mrow><mi>Y</mi><mo>(</mo><mi>V</mi><mo>)</mo></mrow></math></span> was reproduced by assuming a single electron process to excite the C-H stretch mode, and two electron process (ladder climbing of the C-H vibrational levels) and a excitation of the combination band. 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This enabled me to propose a formula for a reaction rate </span></span><span><math><mrow><mi>R</mi><mo>(</mo><mi>V</mi><mo>)</mo></mrow></math></span> or yield per electron <span><math><mrow><mi>Y</mi><mo>(</mo><mi>V</mi><mo>)</mo><mo>=</mo><mi>R</mi><mo>(</mo><mi>V</mi><mo>)</mo><mo>/</mo><mi>I</mi></mrow></math></span>, here <em>I</em> is a tunneling current, <em>i.e.,</em> action spectrum (STM-AS) of a single molecule reaction. I applied this formula to reproduce the experimental result of a CO molecule hopping on Pd (1<!--> <!-->1<!--> <!-->0) surface and more insights into the elementary process were revealed. Thomas Frederiksen and Magus Paulsson jointed me to develop a general formula of <span><math><mrow><mi>Y</mi><mo>(</mo><mi>V</mi><mo>)</mo></mrow></math></span> and successfully applied it to analyse the experimental results of H-atom relay reaction of a linear chain, H(D)<sub>2</sub>O-OH(D)-O(D) H → H(D)-H(D)<sub>2</sub>-OH(D)  → H(D)-H(D)-OH(D)<sub>2</sub><span> that was observed by Takashi Kumagai and Hiroshi Okuyama. Actually a hydrogen atom excited at one end of a linear chain composed of H</span><sub>2</sub>O and several OH generates another one at the other end. We employed our formula of to reproduce the experimental result of <span><math><mrow><mi>Y</mi><mo>(</mo><mi>V</mi><mo>)</mo></mrow></math></span>. It was found that excitation of the three characteristic vibrational modes (free OH/OD stretch, OH<sup>∗</sup> = OD<sup>∗</sup> stretch, and H<sub>2</sub>O scissors, where H<sup>∗</sup> = D<sup>∗</sup> denotes the shared H/D<sup>∗</sup> atom in the H bond) were involved in the relay reaction. It was remarked that the OH(D<sup>∗</sup>) = OD(D<sup>∗</sup><span><span> stretch modes are significantly redshifted from free OH/OD stretch and also characterized by very large broadening. The significant mode softening with respect to the free stretch modes and spectacular enhancement of the width are known to originate in the strong anharmonic character of a single H bond. Thomas investigated the reaction pathway from total energy calculations for the H-atom transfer reaction by the nudged elastic band method. The initial step is translation of the shared H-atom to the center </span>hydroxyl, which is almost barrierless. The subsequent H-bond cleavage between OH and the center water molecule constitutes the highest barrier in which the displacement of the center water molecule along the [0</span> <!-->0<!--> <!-->1] direction is mainly involved. The OH, OH<sup>∗</sup> stretch and H<sub>2</sub>O scissors modes are therefore postulated to couple to the reaction coordinate for the H-bond cleavage. We have demonstrated a vibrationally induced H-atom-bond relay reaction within H-bonded chains assembled on Cu(1<!--> <!-->1<!--> <!-->0). In this reaction H-atom transfer results in the ‘structural’ transfer of a water molecule from one end of the chain to the other end without changing the platform of the chain, or actually transferring the molecule.</p><p>I have been thinking the unresolved issue of C<sub>2</sub>H(D)<sub>2</sub> rotation on Cu (1<!--> <!-->0<!--> <!-->0) since it was published in 1998 by the W. Ho group. 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引用次数: 1

摘要

2001年,我受邀提交了这一个人观点,当时我开始与Maki Kawai教授合作,与Bo Persson一起开发Pd(110)上单个CO分子的横向跳跃理论,我简要描述了我是如何得到金属表面上单个分子振动介导反应的基本过程的想法。在与S.G. Thihodeev教授一起研究非弹性电子隧道能谱(IETS)和扫描隧道能谱(STM-IETS)理论的过程中,我发现IET电流是用单个分子的振动态密度来表示的。这使我提出了反应速率R(V)或每电子产率Y(V)=R(V)/I的公式,这里I是隧穿电流,即单分子反应的作用谱(STM-AS)。我应用这个公式重现了CO分子在Pd(110)表面跳跃的实验结果,揭示了对基本过程的更多认识。Thomas Frederiksen和Magus Paulsson与我共同开发了Y(V)的通式,并成功地应用于熊谷隆和奥山宏观察到的线性链H(D) 20 -OH(D)-O(D) H → H(D)-H(D)2-OH(D) → H(D)-H(D)-OH(D)2的实验结果。实际上,一个氢原子在由H2O和几个OH组成的线性链的一端被激发,在另一端产生另一个。我们用的公式再现了Y(V)的实验结果。发现三种特征振动模式(自由OH/OD拉伸,OH∗ = OD∗拉伸和H2O剪子,其中H∗ = D∗表示H键中共享的H/D∗原子)的激发参与了接力反应。结果表明,OH(D∗) = OD(D∗)的拉伸模式与自由OH/OD拉伸模式有明显的红移,并且具有很大的展宽。相对于自由拉伸模式的显著模式软化和宽度的显著增强是由单个氢键的强非调和特性引起的。Thomas用微推弹性带法从h原子转移反应的总能量计算出发,研究了反应途径。第一步是将共用的h原子转移到中心的羟基上,这几乎是没有障碍的。随后OH与中心水分子之间的氢键劈裂构成了最高位垒,主要涉及中心水分子沿[0 0 1]方向的位移。因此,假设OH, OH *拉伸和H2O剪刀模式与氢键裂解的反应坐标偶联。我们已经证明了在铜(11 10)上组装的h键链中振动诱导的h原子-键接力反应。在该反应中,h原子转移导致水分子从链的一端“结构”转移到另一端,而不改变链的平台,或实际上转移分子。自1998年W. Ho小组发表C2H(D)2在Cu(1 0 0)上的旋转问题以来,我一直在思考这个悬而未决的问题。这种实验方法和结果作为单分子开关的首次演示,被广泛认为是单分子操纵的里程碑式的报道,通过隧道电流和施加偏压来激发分子的振动模式。他们观察到STM图像在施加适当的偏置电压前后以90度旋转。他们进一步比较了IETS光谱和自转的Y(V)。观察到的峰值与阈值偏置电压非常吻合,这清楚地证明了旋转是由C2H(D)2的特定振动模式激发引起的。特别是随着隧穿电流的增加,从单电子过程到双电子过程的交叉是非常有趣的。当时Sergei和他的博士生Yulia E. Shchadilova以及Magnus帮助我重现了所有的实验结果,他们利用Keldysh Green函数理论结合从头算密度泛函数理论(DFT)计算了优化的吸附几何形状,并进行了精密的振动分析。Y(V)的实验结果通过假设一个单电子过程激发C-H拉伸模式,两个电子过程(C-H振动能级的阶梯攀登)和一个组合带的激发得到再现。我还简要介绍了我与Bo、Sergei、Magnus和Thomas共同开发的STM-AS理论。
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Action spectroscopy of single molecules reactions with STM – My personal view back from 2001-

Having obtained an invitation to submit this personal view back to 2001 when I started to work with Prof. Maki Kawai for developing a theory of lateral hopping of a single CO molecule on Pd (1 1 0) with Bo Persson, I briefly describe how I got an idea for elementary processes of vibrationally mediated reactions of single molecules on metal surfaces. During the work with Prof. S.G. Thihodeev on a theory of inelastic electron tunneling spectroscopy (IETS) with scanning tunneling spectrum (STM-IETS), I found that IET current is expressed in terms of a vibrational density of states of a single molecule. This enabled me to propose a formula for a reaction rate R(V) or yield per electron Y(V)=R(V)/I, here I is a tunneling current, i.e., action spectrum (STM-AS) of a single molecule reaction. I applied this formula to reproduce the experimental result of a CO molecule hopping on Pd (1 1 0) surface and more insights into the elementary process were revealed. Thomas Frederiksen and Magus Paulsson jointed me to develop a general formula of Y(V) and successfully applied it to analyse the experimental results of H-atom relay reaction of a linear chain, H(D)2O-OH(D)-O(D) H → H(D)-H(D)2-OH(D)  → H(D)-H(D)-OH(D)2 that was observed by Takashi Kumagai and Hiroshi Okuyama. Actually a hydrogen atom excited at one end of a linear chain composed of H2O and several OH generates another one at the other end. We employed our formula of to reproduce the experimental result of Y(V). It was found that excitation of the three characteristic vibrational modes (free OH/OD stretch, OH = OD stretch, and H2O scissors, where H = D denotes the shared H/D atom in the H bond) were involved in the relay reaction. It was remarked that the OH(D) = OD(D stretch modes are significantly redshifted from free OH/OD stretch and also characterized by very large broadening. The significant mode softening with respect to the free stretch modes and spectacular enhancement of the width are known to originate in the strong anharmonic character of a single H bond. Thomas investigated the reaction pathway from total energy calculations for the H-atom transfer reaction by the nudged elastic band method. The initial step is translation of the shared H-atom to the center hydroxyl, which is almost barrierless. The subsequent H-bond cleavage between OH and the center water molecule constitutes the highest barrier in which the displacement of the center water molecule along the [0 0 1] direction is mainly involved. The OH, OH stretch and H2O scissors modes are therefore postulated to couple to the reaction coordinate for the H-bond cleavage. We have demonstrated a vibrationally induced H-atom-bond relay reaction within H-bonded chains assembled on Cu(1 1 0). In this reaction H-atom transfer results in the ‘structural’ transfer of a water molecule from one end of the chain to the other end without changing the platform of the chain, or actually transferring the molecule.

I have been thinking the unresolved issue of C2H(D)2 rotation on Cu (1 0 0) since it was published in 1998 by the W. Ho group. This experimental methods and the results obtained as the first demonstration of a single molecule switch are widely recognized as a milestone report of a single molecule manipulation by tunneling current and applied bias voltage which excites the vibrational modes of a molecule. They observed the STM images rotated at 90 degrees before and after applying appropriate bias voltage. They further compared the IETS spectrum and the Y(V) for the rotation. The observed peak beautifully agreed with the threshold bias voltage, which clearly evidenced that a rotation is induced by excitation of a particular vibrational mode of C2H(D)2. In particular a crossover from a single electron process to a two electron process with increase in a tunneling current are of great interest. Sergei and his PhD student Yulia E. Shchadilova at that time and Magnus helped me much to reproduce all the experimental results by employing the Keldysh Green’s function theory combined with ab initio density functional theory (DFT) calculation of the optimized adsorption geometry and sophisticated vibrational analysis done by Magus. The experimental result of Y(V) was reproduced by assuming a single electron process to excite the C-H stretch mode, and two electron process (ladder climbing of the C-H vibrational levels) and a excitation of the combination band. I also describe a brief theory of STM-AS I developed with Bo, Sergei, Magnus and Thomas.

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来源期刊
Progress in Surface Science
Progress in Surface Science 工程技术-物理:凝聚态物理
CiteScore
11.30
自引率
0.00%
发文量
10
审稿时长
3 months
期刊介绍: Progress in Surface Science publishes progress reports and review articles by invited authors of international stature. The papers are aimed at surface scientists and cover various aspects of surface science. Papers in the new section Progress Highlights, are more concise and general at the same time, and are aimed at all scientists. Because of the transdisciplinary nature of surface science, topics are chosen for their timeliness from across the wide spectrum of scientific and engineering subjects. The journal strives to promote the exchange of ideas between surface scientists in the various areas. Authors are encouraged to write articles that are of relevance and interest to both established surface scientists and newcomers in the field.
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Editorial Board Current perspective towards a general framework to describe and harness friction at the nanoscale Time-resolved photoemission electron microscopy of semiconductor interfaces Editorial Board Structural dynamics in atomic indium wires on silicon: From ultrafast probing to coherent vibrational control
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