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Photophysics of Nitro-Substituted Unnatural Nucleic Acid Base. 硝基取代的非天然核酸碱基的光物理学。
IF 2.7 2区 化学 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-11-07 Epub Date: 2024-10-29 DOI: 10.1021/acs.jpca.4c03948
Adithya Krishnan Pradeep Kumar, Supriyo Santra, Debashree Ghosh

The unnatural nucleic acid base (uNAB), 6-amino-3-methyl-5-nitropyridin-2(1H)one, often referred to as Z can form a base pair with the uNAB 2-aminoimidazo[1,2-a]-1,3,5-triazin-4(8H)-one (referred to as P) and is analogous to a guanine-cytosine (G-C) pair. However, it is well-known that the nonradiative decay pathway of the P-Z pair is significantly different from that of the G-C pair (Cui et al., Front. Chem. 2020, 8, 605117-605125). In this work, we study the excited state processes in Z using state-of-the-art multireference methods and dynamical techniques to ascertain the predominant nonradiative channels. We find that unlike in the natural NABs, the excited state processes in Z are driven primarily by the -NO2 group rotation. The electron-withdrawing effect of the -NO2 substituent plays a crucial role. We further ascertained that ultrafast deactivation channels are possible in Z and identified the stationary point geometries that are responsible for these channels.

非天然核酸碱基(uNAB)--6-氨基-3-甲基-5-硝基吡啶-2(1H)-酮(通常称为 Z)可与 uNAB 2-氨基咪唑并[1,2-a]-1,3,5-三嗪-4(8H)-酮(称为 P)形成碱基对,类似于鸟嘌呤-胞嘧啶(G-C)对。然而,众所周知,P-Z 对的非辐射衰变途径与 G-C 对有很大不同(Cui 等,Front.)在这项工作中,我们利用最先进的多参量方法和动力学技术研究了 Z 的激发态过程,以确定主要的非辐射通道。我们发现,与天然 NABs 不同,Z 中的激发态过程主要由 -NO2 基团旋转驱动。-NO2取代基的抽电子效应起着至关重要的作用。我们进一步确定了 Z 中可能存在超快失活通道,并确定了造成这些通道的静止点几何结构。
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引用次数: 0
Facilitating Absorption Spectroscopy of Strongly Absorbing Fluids: A High-Throughput Approach. 促进强吸收流体的吸收光谱分析:高通量方法
IF 2.7 2区 化学 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-11-07 Epub Date: 2024-10-24 DOI: 10.1021/acs.jpca.4c04902
Fabian Eller, Eva M Herzig

Measuring absorption spectra of strongly absorbing solutions is usually only possible by diluting the solution. However, the absorption spectra can be heavily influenced by concentration-dependent interactions, so dilution leads to misleading results. To enable reliable absorption measurements of concentrated solutions, we introduce in this work thinning fluid film spectroscopy (TFFS), a simple and highly automatable method. We present three exemplary measurement modes of TFFS suitable for many different applications and validate the TFFS measurements with control data obtained in specialized, low optical path length cuvettes. Additionally, we compare the suitability of the different measurement modes over a broad concentration range and demonstrate the automation possibilities with a spectroscopy robot. Beyond this automated approach for highly efficient and high-throughput lab work, we also show the possibility of direct integration into production systems with an in-line setup, which can be incorporated into a variety of pipe systems. The TFFS method is not limited to samples from material science but can be transferred to a broad variety of research and industry fields, including proteins, food, and pharmaceuticals or also agriculture and forensics.

测量强吸收溶液的吸收光谱通常只能通过稀释溶液来实现。然而,吸收光谱会受到浓度相关性相互作用的严重影响,因此稀释会导致误导性结果。为了能够对浓溶液进行可靠的吸收测量,我们在本研究中介绍了一种简单且高度自动化的方法--稀薄流体膜光谱法(TFFS)。我们介绍了适用于多种不同应用的三种 TFFS 测量模式,并利用在专用低光路长度比色皿中获得的对照数据对 TFFS 测量进行了验证。此外,我们还比较了不同测量模式在广泛浓度范围内的适用性,并演示了使用光谱分析机器人实现自动化的可能性。除了这种用于高效和高通量实验室工作的自动化方法外,我们还展示了将在线装置直接集成到生产系统中的可能性,该装置可集成到各种管道系统中。TFFS 方法并不局限于材料科学领域的样品,还可应用于蛋白质、食品、药品、农业和法医等广泛的研究和工业领域。
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引用次数: 0
Study on Quantum Dynamics of the Na + Na2 Exchanged Reaction and Lifetime Prediction of Na3 Complex Based on the Neural Network Potential Energy Surface. 基于神经网络势能面的 Na + Na2 交换反应量子动力学研究及 Na3 复合物寿命预测
IF 2.7 2区 化学 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-11-07 Epub Date: 2024-10-23 DOI: 10.1021/acs.jpca.4c05712
Jiapeng Zhang, Bayaer Buren, Yongqing Li

A high-precision global potential energy surface (PES) is constructed for the Na3 system based on high-level ab initio calculations and the fundamental invariant neural network (FI-NN) method. The root-mean-square error (RMSE) of the PES is 2.88 cm-1. The state-resolved quantum dynamics of the ground-state Na + Na2 (v = 0, j = 0) → Na2 (v', j') + Na reaction is studied using the time-dependent wave packet (TDWP) method on the new PES. Analysis of the relevant integral cross sections revealed a complicated energy-transfer mechanism during collisions. Similarly, the characteristics of the differential cross sections indicate that the complex-forming mechanism plays a dominant role in the reaction, providing conditions for a comprehensive exploration of the lifetimes of the complexes. Based on the Rice-Ramsperger-Kassel-Marcus (RRKM) theory, the calculated lifetime of the Na3 complex is approximately 3.9 ns.

基于高水平的 ab initio 计算和基本不变神经网络 (FI-NN) 方法,构建了 Na3 体系的高精度全局势能面 (PES)。PES 的均方根误差 (RMSE) 为 2.88 cm-1。在新的 PES 上使用时间相关波包 (TDWP) 方法研究了基态 Na + Na2 (v = 0, j = 0) → Na2 (v', j') + Na 反应的状态分辨量子动力学。对相关积分截面的分析揭示了碰撞过程中复杂的能量传递机制。同样,微分截面的特征也表明复合物形成机制在反应中起着主导作用,这为全面探索复合物的寿命提供了条件。根据 Rice-Ramsperger-Kassel-Marcus (RRKM) 理论,计算出 Na3 复合物的寿命约为 3.9 ns。
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引用次数: 0
Multireference Fock Space Coupled-Cluster Method for the (3,0) Sector. 针对 (3,0) 扇形的多参量福克空间耦合簇方法。
IF 2.7 2区 化学 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-11-07 Epub Date: 2024-10-25 DOI: 10.1021/acs.jpca.4c04357
Monika Musial, Stanisław A Kucharski

This work reports an implementation of a novel realization of the multireference coupled cluster theory formulated in Fock space. Extending the previous formulation carried out in the (1,1) [M. Musial, R. J. Bartlett, J. Chem. Phys. 129, 044101 (2008)], (0,2) [M. Musial, R. J. Bartlett, J. Chem. Phys. 135, 044121 (2011)], and (2,0) [M. Musial, J. Chem. Phys. 136, 134111 (2012)] sectors to the (3,0) sector, we are able to treat structures with three valence electrons. The (3,0) sector describes systems with three electrons added to the reference, which means that in order to perform correlated calculations for the neutral AB molecule, we have to adopt as the reference a triply ionized structure AB3+. A desirable situation occurs when such an ion has a closed-shell structure and also dissociates into closed shell fragments. This feature makes it possible to apply the restricted Hartree-Fock scheme for the whole range of interatomic distances. Examples of molecules of this type are the diatomics formed by the atoms of alkali metals and alkaline earth metals. An analogous structure is also exhibited by alkali metal monocarbides. In the current work, we have calculated the potential energy curves and spectroscopic constants for the LiBe, LiC, and NaC molecules.

这项工作报告了在福克空间中制定的多参量耦合簇理论的新实现。将之前在 (1,1) [M. Musial, R. J. Bartlett, J. Chem. Phys. 129, 044101 (2008)], (0,2) [M. Musial, R. J. Bartlett, J. Chem. Phys. 135, 044121 (2011)] 和 (2,0) [M. Musial, J. Chem. Phys. 136, 134111 (2012)] 扇形中进行的表述扩展到 (3,0) 扇形,我们能够处理具有三个价电子的结构。(3,0)扇区描述的是在参照物上添加三个电子的系统,这意味着为了对中性 AB 分子进行相关计算,我们必须采用三电离结构 AB3+ 作为参照物。当这种离子具有闭壳结构并解离成闭壳碎片时,就会出现理想的情况。这一特征使得在整个原子间距离范围内应用受限哈特里-福克方案成为可能。碱金属和碱土金属原子形成的硅藻土就是这类分子的例子。碱金属单碳化物也表现出类似的结构。在目前的工作中,我们计算了 LiBe、LiC 和 NaC 分子的势能曲线和光谱常数。
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引用次数: 0
Mechanism for Site-Selective Hydroboration of C70 Fullerene with Borane by DFT-D3 Study. 通过 DFT-D3 研究 C70 富勒烯与硼烷的位点选择性氢硼化机制。
IF 2.7 2区 化学 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-11-07 Epub Date: 2024-10-24 DOI: 10.1021/acs.jpca.4c04351
Jong Woan Choi, Bo Mi Kim, Eiji Osawa, Ji Young Lee, Changhoon Lee, Kee Hag Lee
<p><p>We studied the hydroboration of the C<sub>70</sub> fullerene using both B3LYP-D3(BJ)/6-311G(d,p) and M06-2X-D3/6-311G(d,p) levels of theory, incorporating the empirical dispersion interaction, and Fukui index calculations. Potential energy surfaces (PESs) and Gibbs free energy surfaces (GFESs) were calculated for the pathways from four BH<sub>3</sub> adducts (located at the <b><i>AB</i></b>, <b><i>CC</i></b>, <b><i>D</i></b>, and <b><i>E</i></b> sites) on the C<sub>70</sub> to eight products formed by the 1,2-addition of BH<sub>3</sub> across the four [6,6]-ring fused bonds (<b><i>AB</i></b>, <b><i>CC</i></b>, <b><i>DE</i></b>, and <b><i>EE</i></b>) and across the two [5,6]-ring fused bonds (<b><i>AA</i></b> and <b><i>DD</i></b>). These pathways are two-step consecutive reactions. We denoted the positions on the fullerene cage as <b><i>A</i></b> through <i>E</i>, from the pole to the equator, based on the D<sub>5h</sub> symmetry of the C<sub>70</sub> fullerene. In the first step reaction, the product ratios for the four adduct intermediates should be as the primary intermediate BH<sub>3</sub>(<b><i>D</i></b>), the secondary intermediate BH<sub>3</sub>(<b><i>AB</i></b>), the tertiary intermediate BH<sub>3</sub>(<b><i>CC</i></b>), and the minor intermediate BH<sub>3</sub>(<b><i>E</i></b>), based on the Fukui indices. In addition, in the second step reaction, transition states (TSs) from four adduct intermediates to eight product isomers, namely, BH<sub>2</sub>(<b><i>A</i></b>)H (<b><i>B</i></b>) to BH<sub>2</sub>(<b><i>E</i></b>)H (<b><i>E</i></b>), were obtained using the QST2 method. The calculated reaction coordinates showed exothermic reactions for all bonds except the <b><i>EE</i></b> bond. We also confirmed the transition states by frequency calculations and intrinsic reaction coordinate (IRC) analyses. The PESs and GFESs suggest spontaneous processes for the four isomers, of which the primary products are BH<sub>2</sub>(<b><i>A</i></b>)H (<b><i>B</i></b>) and its isomer BH<sub>2</sub>(<b><i>B</i></b>)H (<b><i>A</i></b>), the secondary product is BH<sub>2</sub>(<b><i>C</i></b>)H (<b><i>C</i></b>), and the tertiary product is BH<sub>2</sub>(<b><i>D</i></b>)H (<b><i>D</i></b>), all formed through adduct intermediates. Therefore, through the hydroboration reaction of C<sub>70</sub>, we could predict and design the site selectivity of C<sub>70</sub> by controlling the energy barrier of the transition state in the second step of the reaction. This implies that we could selectively synthesize mainly BH<sub>2</sub>(<b><i>B</i></b>)H (<b><i>A</i></b>) isomers across the AB-[6,6]-ring fused bond and also design BH<sub>2</sub>(<b><i>D</i></b>)H(<b><i>D</i></b>) isomers across the DD-[5,6]-ring fused bond. Also, the calculations of formation rate constants can well simulate the experimental ratio of two C<sub>70</sub>H<sub>2</sub> isomers by the hydrolysis of BH<sub>2</sub>(<b><i>A</i></b>)H(<b><i>B</i></b>), BH<sub>2</sub>(<b><i>B</i></b>)H(<b><i
我们采用 B3LYP-D3(BJ)/6-311G(d,p)和 M06-2X-D3/6-311G(d,p) 理论水平,结合经验弥散相互作用和 Fukui 指数计算,研究了 C70 富勒烯的氢硼化。计算了从 C70 上的四个 BH3 加合物(位于 AB、CC、D 和 E 位点)到由 BH3 通过四个 [6,6]-环熔合键(AB、CC、DE 和 EE)和两个 [5,6]-环熔合键(AA 和 DD)进行 1,2 加成而形成的八个产物的途径的势能面 (PES) 和吉布斯自由能面 (GFES)。这些途径是两步连续反应。根据 C70 富勒烯的 D5h 对称性,我们将富勒烯笼上从极点到赤道的位置命名为 A 至 E。在第一步反应中,根据福井指数,四种加成中间体的产物比率应分别为一级中间体 BH3(D)、二级中间体 BH3(AB)、三级中间体 BH3(CC)和次级中间体 BH3(E)。此外,在第二步反应中,利用 QST2 方法得到了从四个加成中间体到八个产物异构体(即 BH2(A)H (B) 到 BH2(E)H (E))的过渡态(TSs)。计算得出的反应坐标显示,除 EE 键外,所有键都发生了放热反应。我们还通过频率计算和本征反应坐标(IRC)分析确认了过渡态。PES 和 GFES 表明了四种异构体的自发过程,其中一级产物是 BH2(A)H (B) 及其异构体 BH2(B)H (A),二级产物是 BH2(C)H (C),三级产物是 BH2(D)H (D),它们都是通过加成中间体形成的。因此,通过 C70 的氢硼化反应,我们可以通过控制反应第二步中过渡态的能障来预测和设计 C70 的位点选择性。这意味着我们可以选择性地合成主要跨越 AB-[6,6]-ring 熔合键的 BH2(B)H (A) 异构体,也可以设计出跨越 DD-[5,6]-ring 熔合键的 BH2(D)H(D) 异构体。此外,通过计算形成速率常数,可以很好地模拟室温下 BH2(A)H(B)、BH2(B)H(A)和 BH2(C)H(C)产物水解产生两种 C70H2 异构体的实验比例。
{"title":"Mechanism for Site-Selective Hydroboration of C<sub>70</sub> Fullerene with Borane by DFT-D3 Study.","authors":"Jong Woan Choi, Bo Mi Kim, Eiji Osawa, Ji Young Lee, Changhoon Lee, Kee Hag Lee","doi":"10.1021/acs.jpca.4c04351","DOIUrl":"10.1021/acs.jpca.4c04351","url":null,"abstract":"&lt;p&gt;&lt;p&gt;We studied the hydroboration of the C&lt;sub&gt;70&lt;/sub&gt; fullerene using both B3LYP-D3(BJ)/6-311G(d,p) and M06-2X-D3/6-311G(d,p) levels of theory, incorporating the empirical dispersion interaction, and Fukui index calculations. Potential energy surfaces (PESs) and Gibbs free energy surfaces (GFESs) were calculated for the pathways from four BH&lt;sub&gt;3&lt;/sub&gt; adducts (located at the &lt;b&gt;&lt;i&gt;AB&lt;/i&gt;&lt;/b&gt;, &lt;b&gt;&lt;i&gt;CC&lt;/i&gt;&lt;/b&gt;, &lt;b&gt;&lt;i&gt;D&lt;/i&gt;&lt;/b&gt;, and &lt;b&gt;&lt;i&gt;E&lt;/i&gt;&lt;/b&gt; sites) on the C&lt;sub&gt;70&lt;/sub&gt; to eight products formed by the 1,2-addition of BH&lt;sub&gt;3&lt;/sub&gt; across the four [6,6]-ring fused bonds (&lt;b&gt;&lt;i&gt;AB&lt;/i&gt;&lt;/b&gt;, &lt;b&gt;&lt;i&gt;CC&lt;/i&gt;&lt;/b&gt;, &lt;b&gt;&lt;i&gt;DE&lt;/i&gt;&lt;/b&gt;, and &lt;b&gt;&lt;i&gt;EE&lt;/i&gt;&lt;/b&gt;) and across the two [5,6]-ring fused bonds (&lt;b&gt;&lt;i&gt;AA&lt;/i&gt;&lt;/b&gt; and &lt;b&gt;&lt;i&gt;DD&lt;/i&gt;&lt;/b&gt;). These pathways are two-step consecutive reactions. We denoted the positions on the fullerene cage as &lt;b&gt;&lt;i&gt;A&lt;/i&gt;&lt;/b&gt; through &lt;i&gt;E&lt;/i&gt;, from the pole to the equator, based on the D&lt;sub&gt;5h&lt;/sub&gt; symmetry of the C&lt;sub&gt;70&lt;/sub&gt; fullerene. In the first step reaction, the product ratios for the four adduct intermediates should be as the primary intermediate BH&lt;sub&gt;3&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;D&lt;/i&gt;&lt;/b&gt;), the secondary intermediate BH&lt;sub&gt;3&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;AB&lt;/i&gt;&lt;/b&gt;), the tertiary intermediate BH&lt;sub&gt;3&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;CC&lt;/i&gt;&lt;/b&gt;), and the minor intermediate BH&lt;sub&gt;3&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;E&lt;/i&gt;&lt;/b&gt;), based on the Fukui indices. In addition, in the second step reaction, transition states (TSs) from four adduct intermediates to eight product isomers, namely, BH&lt;sub&gt;2&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;A&lt;/i&gt;&lt;/b&gt;)H (&lt;b&gt;&lt;i&gt;B&lt;/i&gt;&lt;/b&gt;) to BH&lt;sub&gt;2&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;E&lt;/i&gt;&lt;/b&gt;)H (&lt;b&gt;&lt;i&gt;E&lt;/i&gt;&lt;/b&gt;), were obtained using the QST2 method. The calculated reaction coordinates showed exothermic reactions for all bonds except the &lt;b&gt;&lt;i&gt;EE&lt;/i&gt;&lt;/b&gt; bond. We also confirmed the transition states by frequency calculations and intrinsic reaction coordinate (IRC) analyses. The PESs and GFESs suggest spontaneous processes for the four isomers, of which the primary products are BH&lt;sub&gt;2&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;A&lt;/i&gt;&lt;/b&gt;)H (&lt;b&gt;&lt;i&gt;B&lt;/i&gt;&lt;/b&gt;) and its isomer BH&lt;sub&gt;2&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;B&lt;/i&gt;&lt;/b&gt;)H (&lt;b&gt;&lt;i&gt;A&lt;/i&gt;&lt;/b&gt;), the secondary product is BH&lt;sub&gt;2&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;C&lt;/i&gt;&lt;/b&gt;)H (&lt;b&gt;&lt;i&gt;C&lt;/i&gt;&lt;/b&gt;), and the tertiary product is BH&lt;sub&gt;2&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;D&lt;/i&gt;&lt;/b&gt;)H (&lt;b&gt;&lt;i&gt;D&lt;/i&gt;&lt;/b&gt;), all formed through adduct intermediates. Therefore, through the hydroboration reaction of C&lt;sub&gt;70&lt;/sub&gt;, we could predict and design the site selectivity of C&lt;sub&gt;70&lt;/sub&gt; by controlling the energy barrier of the transition state in the second step of the reaction. This implies that we could selectively synthesize mainly BH&lt;sub&gt;2&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;B&lt;/i&gt;&lt;/b&gt;)H (&lt;b&gt;&lt;i&gt;A&lt;/i&gt;&lt;/b&gt;) isomers across the AB-[6,6]-ring fused bond and also design BH&lt;sub&gt;2&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;D&lt;/i&gt;&lt;/b&gt;)H(&lt;b&gt;&lt;i&gt;D&lt;/i&gt;&lt;/b&gt;) isomers across the DD-[5,6]-ring fused bond. Also, the calculations of formation rate constants can well simulate the experimental ratio of two C&lt;sub&gt;70&lt;/sub&gt;H&lt;sub&gt;2&lt;/sub&gt; isomers by the hydrolysis of BH&lt;sub&gt;2&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;A&lt;/i&gt;&lt;/b&gt;)H(&lt;b&gt;&lt;i&gt;B&lt;/i&gt;&lt;/b&gt;), BH&lt;sub&gt;2&lt;/sub&gt;(&lt;b&gt;&lt;i&gt;B&lt;/i&gt;&lt;/b&gt;)H(&lt;b&gt;&lt;i","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":" ","pages":"9559-9571"},"PeriodicalIF":2.7,"publicationDate":"2024-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142491182","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Mono- and Bichromophores Formed from Perylene Monoimide Diesters: Competition between Intramolecular Charge Transfer and Intermolecular Singlet Exciton Fission. 由单亚哌啶二酯形成的单双色团:分子内电荷转移与分子间单线激子裂变之间的竞争。
IF 2.7 2区 化学 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-11-07 Epub Date: 2024-10-23 DOI: 10.1021/acs.jpca.4c05424
Demet Demirci Gültekin, Serkan Şen, Ayhan Elmalı, Ahmet Karatay, Muhammet Erkan Köse, Anthony Harriman, Özgür Altan Bozdemir

Perylene monoimide diesters and the corresponding phenyl-linked bichromophores are strongly fluorescent in dilute solution with minimal triplet population after relaxation of the initial Franck-Condon state. The monomer forms nonemissive face-to-face dimers in solution, wherein illumination leads to formation of a spin-correlated, triplet pair with a yield of ca. 13% and with a time constant of 4 ± 1 ps. The triplet pair, which is localized on the aggregate, cannot separate and decays with a mean lifetime of 80 ± 10 ps. The relaxed S1 state of the weakly coupled, phenyl-linked bichromophores establishes an equilibrium with an intramolecular charge-transfer state over a hundred picoseconds or so, depending on the solvent and the geometry of the linkage. This equilibrium mixture, being dominated by the relaxed S1 state, decays on the nanosecond time scale in solution at room temperature without implication of a triplet state. Self-association occurs at higher concentration and, for the para-bridged bichromophore, leads to inefficient triplet formation in tetrahydrofuran at room temperature.

在稀释溶液中,亚珀尔单亚胺二聚体和相应的苯基连接双色荧光团具有强烈的荧光,在初始弗朗克-康顿态松弛后,三重串数量极少。单体在溶液中形成无发射性的面对面二聚体,在光照下会形成自旋相关的三重子对,产量约为 13%,时间常数为 4 ± 1 ps。三重对定位于聚合体上,无法分离,并以 80 ± 10 ps 的平均寿命衰减。根据溶剂和连接几何形状的不同,弱耦合、苯基连接的重色团的松弛 S1 状态与分子内电荷转移状态在一百皮秒左右的时间内达到平衡。这种平衡混合物以松弛的 S1 状态为主,在室温下的溶液中以纳秒级的时间尺度衰减,不会产生三重态。在浓度较高的情况下会发生自结合,对于对位桥接的重色团来说,会导致室温下在四氢呋喃中形成低效率的三重态。
{"title":"Mono- and Bichromophores Formed from Perylene Monoimide Diesters: Competition between Intramolecular Charge Transfer and Intermolecular Singlet Exciton Fission.","authors":"Demet Demirci Gültekin, Serkan Şen, Ayhan Elmalı, Ahmet Karatay, Muhammet Erkan Köse, Anthony Harriman, Özgür Altan Bozdemir","doi":"10.1021/acs.jpca.4c05424","DOIUrl":"10.1021/acs.jpca.4c05424","url":null,"abstract":"<p><p>Perylene monoimide diesters and the corresponding phenyl-linked bichromophores are strongly fluorescent in dilute solution with minimal triplet population after relaxation of the initial Franck-Condon state. The monomer forms nonemissive face-to-face dimers in solution, wherein illumination leads to formation of a spin-correlated, triplet pair with a yield of <i>ca</i>. 13% and with a time constant of 4 ± 1 ps. The triplet pair, which is localized on the aggregate, cannot separate and decays with a mean lifetime of 80 ± 10 ps. The relaxed S<sub>1</sub> state of the weakly coupled, phenyl-linked bichromophores establishes an equilibrium with an intramolecular charge-transfer state over a hundred picoseconds or so, depending on the solvent and the geometry of the linkage. This equilibrium mixture, being dominated by the relaxed S<sub>1</sub> state, decays on the nanosecond time scale in solution at room temperature without implication of a triplet state. Self-association occurs at higher concentration and, for the <i>para</i>-bridged bichromophore, leads to inefficient triplet formation in tetrahydrofuran at room temperature.</p>","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":" ","pages":"9614-9626"},"PeriodicalIF":2.7,"publicationDate":"2024-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11551949/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142491184","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Electric Field Influence on CO Clathrate Hydrates. 电场对一氧化碳凝块水合物的影响。
IF 2.7 2区 化学 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-11-07 Epub Date: 2024-10-23 DOI: 10.1021/acs.jpca.4c05074
Smita Rai, Dhurba Rai

We consider carbon monoxide (CO) confined in the hydrogen-bonded building blocks of sI and sII clathrate hydrates, viz., (512, 51262, 51264) cages, within the density functional theory-based calculations. We study their response to the applied electric fields in terms of changes in the geometrical parameters, dipole moment, HOMO-LUMO gap, and vibrational frequency shift. We examine the stability of CO clathrate hydrate building block cages and identify a possible indication of the field-induced release of CO.

在基于密度泛函理论的计算中,我们考虑了一氧化碳(CO)在 sI 和 sII 克拉水合物氢键构件(即 (512, 51262, 51264) 笼)中的限制。我们从几何参数、偶极矩、HOMO-LUMO 间隙和振动频移的变化角度研究了它们对外加电场的响应。我们研究了一氧化碳水合物结构单元笼的稳定性,并确定了电场诱导一氧化碳释放的可能迹象。
{"title":"Electric Field Influence on CO Clathrate Hydrates.","authors":"Smita Rai, Dhurba Rai","doi":"10.1021/acs.jpca.4c05074","DOIUrl":"10.1021/acs.jpca.4c05074","url":null,"abstract":"<p><p>We consider carbon monoxide (CO) confined in the hydrogen-bonded building blocks of sI and sII clathrate hydrates, viz., (5<sup>12</sup>, 5<sup>12</sup>6<sup>2</sup>, 5<sup>12</sup>6<sup>4</sup>) cages, within the density functional theory-based calculations. We study their response to the applied electric fields in terms of changes in the geometrical parameters, dipole moment, HOMO-LUMO gap, and vibrational frequency shift. We examine the stability of CO clathrate hydrate building block cages and identify a possible indication of the field-induced release of CO.</p>","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":" ","pages":"9596-9605"},"PeriodicalIF":2.7,"publicationDate":"2024-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142491178","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Mixed H2S and H2O Clusters─New Insights into Dispersion-Dominated Hydrogen Bonding. 混合 H2S 和 H2O 簇--对分散主导型氢键的新认识。
IF 2.7 2区 化学 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-11-07 Epub Date: 2024-10-24 DOI: 10.1021/acs.jpca.4c05510
Philipp Meyer, Svenja Jäger, Jai Khatri, Stefan Henkel, Gerhard Schwaab, Martina Havenith

Here, we report the results of an IR spectroscopy study on heteroclusters of H2S and H2O and several of their isotopomers using mass-selective IR spectroscopy in superfluid helium nanodroplets in the range of 2560-2800 cm-1. Based on DFT calculations on the B3LYP-D3/6-311++G(d,p) level of theory, we were able to assign the experimentally observed O-D stretching bands to heterodimer and heterotrimer clusters. Since no bands of the S-H-bound conformer HSH···OH2 could be observed, we were able to determine the O-H-bound conformer HOH···SH2 to be the global minimum structure. A trapping of the local minima in helium nanodroplets was not observed. This is in line with the weaker hydrogen bond expected for H2S complexes. In these clusters, the interaction energy is expected to be more dominated by dispersion and less dictated by highly directional electrostatic forces.

在此,我们报告了在超流体纳米氦液滴中使用质量选择性红外光谱对 H2S 和 H2O 的杂簇及其几种同素异形体在 2560-2800 cm-1 范围内进行红外光谱研究的结果。基于 B3LYP-D3/6-311++G(d,p) 理论水平的 DFT 计算,我们将实验观察到的 O-D 伸展带归属于杂二聚体和杂三聚体簇。由于没有观察到 S-H 结合构象 HSH-OH2 的带,我们确定 O-H 结合构象 HOH-SH2 是全局最小结构。在氦纳米液滴中没有观察到局部最小结构的捕获。这与 H2S 复合物氢键较弱的预期相符。在这些团簇中,相互作用能预计将更多地由分散作用所主导,而较少由高度定向的静电力所决定。
{"title":"Mixed H<sub>2</sub>S and H<sub>2</sub>O Clusters─New Insights into Dispersion-Dominated Hydrogen Bonding.","authors":"Philipp Meyer, Svenja Jäger, Jai Khatri, Stefan Henkel, Gerhard Schwaab, Martina Havenith","doi":"10.1021/acs.jpca.4c05510","DOIUrl":"10.1021/acs.jpca.4c05510","url":null,"abstract":"<p><p>Here, we report the results of an IR spectroscopy study on heteroclusters of H<sub>2</sub>S and H<sub>2</sub>O and several of their isotopomers using mass-selective IR spectroscopy in superfluid helium nanodroplets in the range of 2560-2800 cm<sup>-1</sup>. Based on DFT calculations on the B3LYP-D3/6-311++G(d,p) level of theory, we were able to assign the experimentally observed O-D stretching bands to heterodimer and heterotrimer clusters. Since no bands of the S-H-bound conformer HSH···OH<sub>2</sub> could be observed, we were able to determine the O-H-bound conformer HOH···SH<sub>2</sub> to be the global minimum structure. A trapping of the local minima in helium nanodroplets was not observed. This is in line with the weaker hydrogen bond expected for H<sub>2</sub>S complexes. In these clusters, the interaction energy is expected to be more dominated by dispersion and less dictated by highly directional electrostatic forces.</p>","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":" ","pages":"9627-9633"},"PeriodicalIF":2.7,"publicationDate":"2024-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142491183","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Rate Constants of the H + HCF3 → H2 + CF3 Reaction from Ring Polymer Molecular Dynamics on a Highly Accurate Potential Energy Surface. 高精度势能面上环状聚合物分子动力学得出的 H + HCF3 → H2 + CF3 反应速率常数。
IF 2.7 2区 化学 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-11-07 Epub Date: 2024-10-29 DOI: 10.1021/acs.jpca.4c05352
Yongfa Zhu, Hongwei Song

The reaction between H and HCF3 is the primary consumption pathway of HCF3 in the atmosphere and combustion. In this work, ring polymer molecular dynamics (RPMD) calculations are performed to calculate the rate constants of the reaction on a recently developed accurate potential energy surface. 36, 20, and 8 beads are used to compute the rate constants at 350 K ≤ T < 800 K, 800 K ≤ T ≤ 1000 K, and T > 1000 K, respectively. The obtained RPMD rate constants agree well with the experimental measurements. In addition, a detailed analysis of the free-energy curves and transmission coefficients reveals that the quantum tunneling significantly affects the reaction dynamics, even at high temperatures.

H 与 HCF3 之间的反应是大气和燃烧中 HCF3 的主要消耗途径。在这项工作中,通过环聚合物分子动力学(RPMD)计算,在最近开发的精确势能面上计算出了反应的速率常数。在 350 K ≤ T < 800 K、800 K ≤ T ≤ 1000 K 和 T > 1000 K 条件下,分别使用 36、20 和 8 个珠子计算速率常数。所得到的 RPMD 速率常数与实验测量结果非常吻合。此外,对自由能曲线和传输系数的详细分析显示,量子隧道对反应动力学有显著影响,即使在高温下也是如此。
{"title":"Rate Constants of the H + HCF<sub>3</sub> → H<sub>2</sub> + CF<sub>3</sub> Reaction from Ring Polymer Molecular Dynamics on a Highly Accurate Potential Energy Surface.","authors":"Yongfa Zhu, Hongwei Song","doi":"10.1021/acs.jpca.4c05352","DOIUrl":"10.1021/acs.jpca.4c05352","url":null,"abstract":"<p><p>The reaction between H and HCF<sub>3</sub> is the primary consumption pathway of HCF<sub>3</sub> in the atmosphere and combustion. In this work, ring polymer molecular dynamics (RPMD) calculations are performed to calculate the rate constants of the reaction on a recently developed accurate potential energy surface. 36, 20, and 8 beads are used to compute the rate constants at 350 K ≤ <i>T</i> < 800 K, 800 K ≤ <i>T</i> ≤ 1000 K, and <i>T</i> > 1000 K, respectively. The obtained RPMD rate constants agree well with the experimental measurements. In addition, a detailed analysis of the free-energy curves and transmission coefficients reveals that the quantum tunneling significantly affects the reaction dynamics, even at high temperatures.</p>","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":" ","pages":"9606-9613"},"PeriodicalIF":2.7,"publicationDate":"2024-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142520268","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Diagrams in Polaritonic Coupled Cluster Theory. 极性耦合簇理论中的图表
IF 2.7 2区 化学 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-11-07 Epub Date: 2024-10-23 DOI: 10.1021/acs.jpca.4c04389
Laurenz Monzel, Stella Stopkowicz

We present a diagrammatic notation to derive the quantum-electrodynamic coupled cluster (QED-CC) equations needed for the description for polaritonic ground and excited states. Our presented notation is a generalization of the existing diagrammatic notation of standard electronic coupled-cluster theory. It is used to derive the QED-CC and QED-EOM-CC equations for the QED-CCSD-1-SD and QED-CCSD-12-SD truncation schemes. Furthermore, we present the diagrams for the CC Λ-equations and reduced density matrices which are needed for the calculation of molecular properties.

我们提出了一种图解符号,用于推导描述极性基态和激发态所需的量子电动力学耦合簇(QED-CC)方程。我们提出的符号是对标准电子耦合簇理论现有图解符号的概括。它用于推导 QED-CCSD-1-SD 和 QED-CCSD-12-SD 截断方案的 QED-CC 和 QED-EOM-CC 方程。此外,我们还提出了计算分子性质所需的 CC Λ方程和还原密度矩阵图。
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The Journal of Physical Chemistry A
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