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。
{"title":"Photophysics of Nitro-Substituted Unnatural Nucleic Acid Base.","authors":"Adithya Krishnan Pradeep Kumar, Supriyo Santra, Debashree Ghosh","doi":"10.1021/acs.jpca.4c03948","DOIUrl":"10.1021/acs.jpca.4c03948","url":null,"abstract":"<p><p>The unnatural nucleic acid base (uNAB), 6-amino-3-methyl-5-nitropyridin-2(1H)one, often referred to as <i>Z</i> can form a base pair with the uNAB 2-aminoimidazo[1,2-<i>a</i>]-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., <i>Front. Chem.</i> <b>2020</b>, <i>8</i>, 605117-605125). In this work, we study the excited state processes in <i>Z</i> 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 <i>Z</i> are driven primarily by the -NO<sub>2</sub> group rotation. The electron-withdrawing effect of the -NO<sub>2</sub> substituent plays a crucial role. We further ascertained that ultrafast deactivation channels are possible in <i>Z</i> and identified the stationary point geometries that are responsible for these channels.</p>","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":" ","pages":"9551-9558"},"PeriodicalIF":2.7,"publicationDate":"2024-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142542917","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}
Pub Date : 2024-11-07Epub Date: 2024-10-24DOI: 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.
{"title":"Facilitating Absorption Spectroscopy of Strongly Absorbing Fluids: A High-Throughput Approach.","authors":"Fabian Eller, Eva M Herzig","doi":"10.1021/acs.jpca.4c04902","DOIUrl":"10.1021/acs.jpca.4c04902","url":null,"abstract":"<p><p>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.</p>","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":" ","pages":"9682-9687"},"PeriodicalIF":2.7,"publicationDate":"2024-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142491180","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}
Pub Date : 2024-11-07Epub Date: 2024-10-23DOI: 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。
{"title":"Study on Quantum Dynamics of the Na + Na<sub>2</sub> Exchanged Reaction and Lifetime Prediction of Na<sub>3</sub> Complex Based on the Neural Network Potential Energy Surface.","authors":"Jiapeng Zhang, Bayaer Buren, Yongqing Li","doi":"10.1021/acs.jpca.4c05712","DOIUrl":"10.1021/acs.jpca.4c05712","url":null,"abstract":"<p><p>A high-precision global potential energy surface (PES) is constructed for the Na<sub>3</sub> system based on high-level <i>ab initio</i> calculations and the fundamental invariant neural network (FI-NN) method. The root-mean-square error (RMSE) of the PES is 2.88 cm<sup>-1</sup>. The state-resolved quantum dynamics of the ground-state Na + Na<sub>2</sub> (<i>v</i> = 0, <i>j</i> = 0) → Na<sub>2</sub> (<i>v</i>', <i>j</i>') + 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 Na<sub>3</sub> complex is approximately 3.9 ns.</p>","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":" ","pages":"9634-9644"},"PeriodicalIF":2.7,"publicationDate":"2024-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142491188","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}
Pub Date : 2024-11-07Epub Date: 2024-10-25DOI: 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。
{"title":"Multireference Fock Space Coupled-Cluster Method for the (3,0) Sector.","authors":"Monika Musial, Stanisław A Kucharski","doi":"10.1021/acs.jpca.4c04357","DOIUrl":"10.1021/acs.jpca.4c04357","url":null,"abstract":"<p><p>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. <b>129</b>, 044101 (2008)], (0,2) [M. Musial, R. J. Bartlett, J. Chem. Phys. <b>135</b>, 044121 (2011)], and (2,0) [M. Musial, J. Chem. Phys. <b>136</b>, 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 <i>AB</i> molecule, we have to adopt as the reference a triply ionized structure <i>AB</i><sup>3+</sup>. 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.</p>","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":" ","pages":"9670-9681"},"PeriodicalIF":2.7,"publicationDate":"2024-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11551963/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142491185","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}
Pub Date : 2024-11-07Epub Date: 2024-10-24DOI: 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
{"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":"<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","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}
Pub Date : 2024-11-07Epub Date: 2024-10-23DOI: 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.
{"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}
Pub Date : 2024-11-07Epub Date: 2024-10-23DOI: 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}
Pub Date : 2024-11-07Epub Date: 2024-10-24DOI: 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.
{"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}
Pub Date : 2024-11-07Epub Date: 2024-10-29DOI: 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}
Pub Date : 2024-11-07Epub Date: 2024-10-23DOI: 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.
{"title":"Diagrams in Polaritonic Coupled Cluster Theory.","authors":"Laurenz Monzel, Stella Stopkowicz","doi":"10.1021/acs.jpca.4c04389","DOIUrl":"10.1021/acs.jpca.4c04389","url":null,"abstract":"<p><p>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.</p>","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":" ","pages":"9572-9586"},"PeriodicalIF":2.7,"publicationDate":"2024-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142491176","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}