The ground state and excited state resonance dipole-dipole interaction energy between two elongated conducting molecules is explored in this study. We review the current status for ground state interactions. This interaction is found to be of a much longer range than in the case when the molecules are pointlike and nonconducting. These are well known results found earlier by Davies, Ninham, and Richmond, and later, using a different formalism, by Rubio and co-workers. We show how the theory can be extended to excited state interactions. A characteristic property observed from our calculation is that the interaction energy dependence on separation (R) follows f(R)/R2 for both resonance and van der Waals cases in the long-range limit. Under some limits, f(R) has a logarithmic dependency, while under others, it has constant values. We predict an unusual slow decay rate for the energy transfer between conducting molecules.
{"title":"Dispersion interaction between thin conducting cylinders.","authors":"Subhojit Pal, Iver Brevik, Mathias Boström","doi":"10.1039/d4cp01664e","DOIUrl":"10.1039/d4cp01664e","url":null,"abstract":"<p><p>The ground state and excited state resonance dipole-dipole interaction energy between two elongated conducting molecules is explored in this study. We review the current status for ground state interactions. This interaction is found to be of a much longer range than in the case when the molecules are pointlike and nonconducting. These are well known results found earlier by Davies, Ninham, and Richmond, and later, using a different formalism, by Rubio and co-workers. We show how the theory can be extended to excited state interactions. A characteristic property observed from our calculation is that the interaction energy dependence on separation (<i>R</i>) follows <i>f</i>(<i>R</i>)/<i>R</i><sup>2</sup> for both resonance and van der Waals cases in the long-range limit. Under some limits, <i>f</i>(<i>R</i>) has a logarithmic dependency, while under others, it has constant values. We predict an unusual slow decay rate for the energy transfer between conducting molecules.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":null,"pages":null},"PeriodicalIF":2.9,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141416735","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Hachem Araji, Maria Nakhoul, Elio Challita, Nour Barmo, Brigitte Wex
Pyrene and acene derivatives are an important source of materials for optoelectronic device applications both as emitters and organic semiconductors. The mobility of major charge carriers is correlated with the coupling constants of the respective major charge carrier as well as the relaxation energies. Herein, we have applied range-separated density functionals for the estimation of said values. A series of five alkylated derivatives of pyrene laterally extended by heteroaromatic or phenyl groups were explored and contrasted to nascent pyrene, alkylated pyrene and tetracene. The ground state geometries along with absorption properties and relaxation energies are presented as well as a discussion of the suitability of the material toward hole and electron transport materials.
{"title":"Cross-over from pyrene to acene optical and electronic properties: a theoretical investigation of a series of pyrene derivatives fused with N-, S, and O-containing heterocycles.","authors":"Hachem Araji, Maria Nakhoul, Elio Challita, Nour Barmo, Brigitte Wex","doi":"10.1039/d4cp01625d","DOIUrl":"10.1039/d4cp01625d","url":null,"abstract":"<p><p>Pyrene and acene derivatives are an important source of materials for optoelectronic device applications both as emitters and organic semiconductors. The mobility of major charge carriers is correlated with the coupling constants of the respective major charge carrier as well as the relaxation energies. Herein, we have applied range-separated density functionals for the estimation of said values. A series of five alkylated derivatives of pyrene laterally extended by heteroaromatic or phenyl groups were explored and contrasted to nascent pyrene, alkylated pyrene and tetracene. The ground state geometries along with absorption properties and relaxation energies are presented as well as a discussion of the suitability of the material toward hole and electron transport materials.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":null,"pages":null},"PeriodicalIF":2.9,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141445629","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The structures, stability, and electrochemical performances of Janus Ti2BST (T = O, Se) monolayers as anode materials for Na/K-ion batteries (NIBs/KIBs) are investigated by first-principles calculations. The results demonstrate that Ti2BST monolayers are mechanically, dynamically, and thermally stable. The electronic structures display good conductivity. Moreover, the low diffusion barriers of 0.107/0.039 eV (0.111/0.063 eV) for Na/K indicate that the Ti2BSO (Ti2BSSe) monolayer has excellent rate performance for NIBs/KIBs. Low average open circuit voltages (OCVs) (0.322-0.439 V) can produce a high voltage in NIBs/KIBs. Meanwhile, little structural changes during charge/discharge ensure great cycle stability. Especially, the Ti2BSO monolayer has a high theoretical capacity of 691.64/537.75 mA h g-1 for NIBs/KIBs. The outstanding performances demonstrate that the Ti2BST monolayers are potential anode materials for NIBs/KIBs.
{"title":"Theoretical investigation of Janus Ti<sub>2</sub>BST (T = O, Se) monolayers as anode materials for Na/K-ion batteries.","authors":"Yanzong Wang, Lili Xie, Rui Huang, Sai Yan, Xingyong Xie, Qinfang Zhang","doi":"10.1039/d4cp01188k","DOIUrl":"10.1039/d4cp01188k","url":null,"abstract":"<p><p>The structures, stability, and electrochemical performances of Janus Ti<sub>2</sub>BST (T = O, Se) monolayers as anode materials for Na/K-ion batteries (NIBs/KIBs) are investigated by first-principles calculations. The results demonstrate that Ti<sub>2</sub>BST monolayers are mechanically, dynamically, and thermally stable. The electronic structures display good conductivity. Moreover, the low diffusion barriers of 0.107/0.039 eV (0.111/0.063 eV) for Na/K indicate that the Ti<sub>2</sub>BSO (Ti<sub>2</sub>BSSe) monolayer has excellent rate performance for NIBs/KIBs. Low average open circuit voltages (OCVs) (0.322-0.439 V) can produce a high voltage in NIBs/KIBs. Meanwhile, little structural changes during charge/discharge ensure great cycle stability. Especially, the Ti<sub>2</sub>BSO monolayer has a high theoretical capacity of 691.64/537.75 mA h g<sup>-1</sup> for NIBs/KIBs. The outstanding performances demonstrate that the Ti<sub>2</sub>BST monolayers are potential anode materials for NIBs/KIBs.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":null,"pages":null},"PeriodicalIF":2.9,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141441852","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Tetsuroh Shirasawa, Wolfgang Voegeli, Etsuo Arakawa
X-ray absorption spectroscopy (XAS) and small-angle X-ray scattering (SAXS) are common materials characterization tools at synchrotron radiation facilities used in many research fields. Since XAS can provide element-specific chemical states and local atomic structures and SAXS can provide nano-scale structural information, their complementary use is advantageous for a comprehensive understanding of multiscale phenomena. This paper presents a new method for simultaneous XAS/SAXS measurements with synchrotron radiation. The method employs a polychromatic X-ray beam as in the energy-dispersive XAS technique and captures both the transmission XAS spectrum and the SAXS intensity distribution with an area X-ray detector, which eliminates the energy scan in the conventional methods and realizes the simultaneous data acquisition in a shorter time. We succeeded in obtaining the atomic and nano-scale structures of Pt and Pt/Pd nanoparticles with a data acquisition time of 0.1 s, suggesting the potential for real-time observation of multiscale phenomena.
X 射线吸收光谱(XAS)和小角 X 射线散射(SAXS)是同步辐射设施中常用的材料表征工具,可用于许多研究领域。由于 XAS 可以提供特定元素的化学状态和局部原子结构,而 SAXS 可以提供纳米尺度的结构信息,因此二者的互补使用有利于全面了解多尺度现象。本文介绍了一种利用同步辐射同时测量 XAS/SAXS 的新方法。该方法采用了能量色散 XAS 技术中的多色 X 射线束,并通过一个面积 X 射线探测器同时捕获透射 XAS 光谱和 SAXS 强度分布,从而省去了传统方法中的能量扫描,在更短的时间内实现了同步数据采集。我们成功地在 0.1 秒的数据采集时间内获得了铂和铂/钯纳米粒子的原子和纳米尺度结构,为实时观测多尺度现象提供了可能。
{"title":"Simultaneous fast XAS/SAXS measurements in an energy-dispersive mode.","authors":"Tetsuroh Shirasawa, Wolfgang Voegeli, Etsuo Arakawa","doi":"10.1039/d4cp01399a","DOIUrl":"10.1039/d4cp01399a","url":null,"abstract":"<p><p>X-ray absorption spectroscopy (XAS) and small-angle X-ray scattering (SAXS) are common materials characterization tools at synchrotron radiation facilities used in many research fields. Since XAS can provide element-specific chemical states and local atomic structures and SAXS can provide nano-scale structural information, their complementary use is advantageous for a comprehensive understanding of multiscale phenomena. This paper presents a new method for simultaneous XAS/SAXS measurements with synchrotron radiation. The method employs a polychromatic X-ray beam as in the energy-dispersive XAS technique and captures both the transmission XAS spectrum and the SAXS intensity distribution with an area X-ray detector, which eliminates the energy scan in the conventional methods and realizes the simultaneous data acquisition in a shorter time. We succeeded in obtaining the atomic and nano-scale structures of Pt and Pt/Pd nanoparticles with a data acquisition time of 0.1 s, suggesting the potential for real-time observation of multiscale phenomena.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":null,"pages":null},"PeriodicalIF":2.9,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141445630","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Svetlana Tsizin, Loren Ban, Egor Chasovskikh, Bruce L Yoder, Ruth Signorell
An oxybenzone molecule in the gas phase was characterized by mass spectrometry and angle-resolved photoelectron spectroscopy, using both single and multiphoton ionization schemes. A tabletop high harmonic generation source with a monochromator was used for single-photon ionization of oxybenzone with photon energies of up to 35.7 eV. From this, vertical ionization and appearance energies, as well as energy-dependent anisotropy parameters were retrieved and compared with the results from DFT calculations. For two-photon ionization using 4.7 eV light, we found a higher appearance energy than in the extreme ultraviolet (EUV) case, highlighting the possible influence of an intermediate state on the photoionization process. We found no differences in the mass spectra when ionizing oxybenzone by single-photons between 17.2 and 35.7 eV. However, for the multiphoton ionization, the fragmentation process was found to be sensitive to the photoionization order and laser intensity. The "softest" method was found to be two-photon ionization using 4.7 eV light, which led to no measurable fragmentation up to an intensity of 5 × 1012 W cm-2.
利用单光子和多光子电离方案,通过质谱法和角度分辨光电子能谱法对气相中的氧苯酮分子进行了表征。使用带有单色器的台式高次谐波发生源对羟苯酮进行单光子电离,光子能量高达 35.7 eV。由此获得了垂直电离和外观能量,以及随能量变化的各向异性参数,并与 DFT 计算结果进行了比较。对于使用 4.7 eV 光的双光子电离,我们发现其外观能高于极紫外(EUV)情况下的外观能,这凸显了中间状态对光离子化过程的可能影响。我们发现,在 17.2 至 35.7 eV 之间用单光子电离羟苯酮时,质谱没有差异。然而,在多光子电离中,我们发现碎裂过程对光离子化顺序和激光强度很敏感。最 "柔和 "的方法是使用 4.7 eV 光的双光子电离,这种方法在 5 × 1012 W cm-2 的强度下不会产生可测量的碎片。
{"title":"Valence photoelectron imaging of molecular oxybenzone.","authors":"Svetlana Tsizin, Loren Ban, Egor Chasovskikh, Bruce L Yoder, Ruth Signorell","doi":"10.1039/d3cp06224d","DOIUrl":"https://doi.org/10.1039/d3cp06224d","url":null,"abstract":"<p><p>An oxybenzone molecule in the gas phase was characterized by mass spectrometry and angle-resolved photoelectron spectroscopy, using both single and multiphoton ionization schemes. A tabletop high harmonic generation source with a monochromator was used for single-photon ionization of oxybenzone with photon energies of up to 35.7 eV. From this, vertical ionization and appearance energies, as well as energy-dependent anisotropy parameters were retrieved and compared with the results from DFT calculations. For two-photon ionization using 4.7 eV light, we found a higher appearance energy than in the extreme ultraviolet (EUV) case, highlighting the possible influence of an intermediate state on the photoionization process. We found no differences in the mass spectra when ionizing oxybenzone by single-photons between 17.2 and 35.7 eV. However, for the multiphoton ionization, the fragmentation process was found to be sensitive to the photoionization order and laser intensity. The \"softest\" method was found to be two-photon ionization using 4.7 eV light, which led to no measurable fragmentation up to an intensity of 5 × 10<sup>12</sup> W cm<sup>-2</sup>.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":null,"pages":null},"PeriodicalIF":2.9,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141490050","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Simon Bacon, Shumaila Babar, Matthew Dent, Allan Foster, Joseph Paul Baboo, Teng Zhang, John F Watts, Constantina Lekakou
The present investigation fits the reaction kinetics of a lithium-sulfur (Li-S) battery with polar electrolyte employing a novel two-phase continuum multipore model. The continuum two-phase model considers processes in both the liquid electrolyte phase and the solid precipitates phase, where the diffusion coefficients of the Li+ ions in a solvent-softened solid state are determined from molecular dynamics simulations. Solubility experiments yield the saturation concentration of sulfur and lithium sulfides in the polar electrolyte employed in this study. The model describes the transport of dissolved molecular and ion species in pores of different size in solvated or desolvated form, depending on pore size. The Li-S reaction model in this study is validated for electrolyte 1 M LiPF6 in EC/DMC. It includes seven redox reactions and two cyclic non-electrochemical reactions in the cathode, and the lithium redox reaction at the anode. Electrochemical reactions are assumed to take place in the electrolyte solution or the solid state and cyclic reactions are assumed to take place in the liquid electrolyte phase only. The determination of the reaction kinetics parameters takes place via fitting the model predictions with experimental data of a cyclic voltammetry cycle with in operando UV-vis spectroscopy.
本研究采用新型两相连续多孔模型拟合了极性电解质锂硫(Li-S)电池的反应动力学。连续两相模型考虑了液态电解质相和固态沉淀相的过程,其中锂+ 离子在溶剂软化固态中的扩散系数是通过分子动力学模拟确定的。溶解度实验得出了本研究采用的极性电解质中硫和硫化锂的饱和浓度。该模型描述了溶解的分子和离子物种在不同大小的孔隙中以溶解或去溶解的形式(取决于孔隙大小)进行的传输。本研究中的锂-S 反应模型针对 EC/DMC 中的 1 M LiPF6 电解质进行了验证。它包括阴极的七个氧化还原反应和两个循环非电化学反应,以及阳极的锂氧化还原反应。电化学反应假定发生在电解质溶液或固态中,循环反应假定只发生在液态电解质阶段。反应动力学参数的确定是通过将模型预测与循环伏安法周期的实验数据进行拟合,并结合操作中的紫外-可见光谱来实现的。
{"title":"Reaction kinetics of lithium-sulfur batteries with a polar Li-ion electrolyte: modeling of liquid phase and solid phase processes.","authors":"Simon Bacon, Shumaila Babar, Matthew Dent, Allan Foster, Joseph Paul Baboo, Teng Zhang, John F Watts, Constantina Lekakou","doi":"10.1039/d4cp02061h","DOIUrl":"https://doi.org/10.1039/d4cp02061h","url":null,"abstract":"<p><p>The present investigation fits the reaction kinetics of a lithium-sulfur (Li-S) battery with polar electrolyte employing a novel two-phase continuum multipore model. The continuum two-phase model considers processes in both the liquid electrolyte phase and the solid precipitates phase, where the diffusion coefficients of the Li<sup>+</sup> ions in a solvent-softened solid state are determined from molecular dynamics simulations. Solubility experiments yield the saturation concentration of sulfur and lithium sulfides in the polar electrolyte employed in this study. The model describes the transport of dissolved molecular and ion species in pores of different size in solvated or desolvated form, depending on pore size. The Li-S reaction model in this study is validated for electrolyte 1 M LiPF<sub>6</sub> in EC/DMC. It includes seven redox reactions and two cyclic non-electrochemical reactions in the cathode, and the lithium redox reaction at the anode. Electrochemical reactions are assumed to take place in the electrolyte solution or the solid state and cyclic reactions are assumed to take place in the liquid electrolyte phase only. The determination of the reaction kinetics parameters takes place <i>via</i> fitting the model predictions with experimental data of a cyclic voltammetry cycle with <i>in operando</i> UV-vis spectroscopy.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":null,"pages":null},"PeriodicalIF":2.9,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141490049","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Ginny Karir, Enrique Mendez-Vega, Adrian Portela-Gonzalez, Mayank Saraswat, Wolfram Sander, Patrick Hemberger
Alkynyl radicals and cations are crucial reactive intermediates in chemistry, but often evade direct detection. Herein, we report the direct observation of the phenylethynyl radical (C6H5CC˙) and its cation (C6H5CC+), which are two of the most reactive intermediates in organic chemistry. The radical is generated via pyrolysis of (bromoethynyl)benzene at temperatures above 1500 K and is characterized by photoion mass-selected threshold photoelectron spectroscopy (ms-TPES). Photoionization of the phenylethynyl radical yields the phenylethynyl cation, which has never been synthesized due to its extreme electrophilicity. Vibrationally-resolved ms-TPES assisted by ab initio calculations unveiled the complex electronic structure of the phenylethynyl cation, which appears at an adiabatic ionization energy (AIE) of 8.90 ± 0.05 eV and exhibits an uncommon triplet (3B1) ground state, while the closed-shell singlet (1A1) state lies just 2.8 kcal mol-1 (0.12 eV) higher in energy. The reactive phenylethynyl radical abstracts hydrogen to form ethynylbenzene (C6H5CCH) but also isomerizes via H-shift to the o-, m-, and p-ethynylphenyl isomers (C6H4CCH). These radicals are very reactive and undergo ring-opening followed by H-loss to form a mixture of C8H4 triynes, along with low yields of cyclic 3- and 4-ethynylbenzynes (C6H3CCH). At higher temperatures, dehydrogenation from the unbranched C8H4 triynes forms the linear tetraacetylene (C8H2), an astrochemically relevant polyyne.
炔基和阳离子是化学中重要的反应中间体,但往往无法直接检测。在本文中,我们报告了对苯乙炔基(C6H5CC˙)及其阳离子(C6H5CC+)的直接观察,它们是有机化学中最活跃的两种中间体。该自由基是通过(溴乙炔基)苯在高于 1500 K 的温度下热解生成的,并通过光离子质量选择阈值光电子能谱(ms-TPES)进行表征。苯乙炔基的光离子化产生了苯乙炔阳离子,由于其极度亲电性,这种阳离子从未被合成过。振荡分辨 ms-TPES 和 ab initio 计算揭示了苯乙炔阳离子的复杂电子结构,其绝热电离能 (AIE) 为 8.90 ± 0.05 eV,表现出不常见的三重态 (3B1) 基态,而闭壳单重态 (1A1) 的能量仅高出 2.8 kcal mol-1 (0.12 eV)。活性苯乙炔基汲取氢形成乙炔苯(C6H5CCH),但也会通过 H 移位异构化成邻、间和对乙炔苯基异构体(C6H4CCH)。这些自由基非常活泼,在开环后会发生 H 损失,形成 C8H4 三炔混合物,以及产量较低的环状 3-和 4-乙炔基苄(C6H3CCH)。在较高温度下,未支化的 C8H4 三炔脱氢形成线性四乙炔(C8H2),这是一种与天体化学有关的聚炔。
{"title":"The elusive phenylethynyl radical and its cation: synthesis, electronic structure, and reactivity.","authors":"Ginny Karir, Enrique Mendez-Vega, Adrian Portela-Gonzalez, Mayank Saraswat, Wolfram Sander, Patrick Hemberger","doi":"10.1039/d4cp02129k","DOIUrl":"10.1039/d4cp02129k","url":null,"abstract":"<p><p>Alkynyl radicals and cations are crucial reactive intermediates in chemistry, but often evade direct detection. Herein, we report the direct observation of the phenylethynyl radical (C<sub>6</sub>H<sub>5</sub>CC˙) and its cation (C<sub>6</sub>H<sub>5</sub>CC<sup>+</sup>), which are two of the most reactive intermediates in organic chemistry. The radical is generated <i>via</i> pyrolysis of (bromoethynyl)benzene at temperatures above 1500 K and is characterized by photoion mass-selected threshold photoelectron spectroscopy (ms-TPES). Photoionization of the phenylethynyl radical yields the phenylethynyl cation, which has never been synthesized due to its extreme electrophilicity. Vibrationally-resolved ms-TPES assisted by <i>ab initio</i> calculations unveiled the complex electronic structure of the phenylethynyl cation, which appears at an adiabatic ionization energy (AIE) of 8.90 ± 0.05 eV and exhibits an uncommon triplet (<sup>3</sup>B<sub>1</sub>) ground state, while the closed-shell singlet (<sup>1</sup>A<sub>1</sub>) state lies just 2.8 kcal mol<sup>-1</sup> (0.12 eV) higher in energy. The reactive phenylethynyl radical abstracts hydrogen to form ethynylbenzene (C<sub>6</sub>H<sub>5</sub>CCH) but also isomerizes <i>via</i> H-shift to the <i>o</i>-, <i>m</i>-, and <i>p</i>-ethynylphenyl isomers (C<sub>6</sub>H<sub>4</sub>CCH). These radicals are very reactive and undergo ring-opening followed by H-loss to form a mixture of C<sub>8</sub>H<sub>4</sub> triynes, along with low yields of cyclic 3- and 4-ethynylbenzynes (C<sub>6</sub>H<sub>3</sub>CCH). At higher temperatures, dehydrogenation from the unbranched C<sub>8</sub>H<sub>4</sub> triynes forms the linear tetraacetylene (C<sub>8</sub>H<sub>2</sub>), an astrochemically relevant polyyne.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":null,"pages":null},"PeriodicalIF":2.9,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141430909","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Shane J Goettl, Chao He, Zhenghai Yang, Ralf I Kaiser, Ankit Somani, Adrian Portela-Gonzalez, Wolfram Sander, Bing-Jian Sun, Siti Fatimah, Komal P Kadam, Agnes H H Chang
The biphenyl molecule (C12H10) acts as a fundamental molecular backbone in the stereoselective synthesis of organic materials due to its inherent twist angle causing atropisomerism in substituted derivatives and in molecular mass growth processes in circumstellar environments and combustion systems. Here, we reveal an unconventional low-temperature phenylethynyl addition-cyclization-aromatization mechanism for the gas-phase preparation of biphenyl (C12H10) along with ortho-, meta-, and para-substituted methylbiphenyl (C13H12) derivatives through crossed molecular beams and computational studies providing compelling evidence on their formation via bimolecular gas-phase reactions of phenylethynyl radicals (C6H5CC, X2A1) with 1,3-butadiene-d6 (C4D6), isoprene (CH2C(CH3)CHCH2), and 1,3-pentadiene (CH2CHCHCHCH3). The dynamics involve de-facto barrierless phenylethynyl radical additions via submerged barriers followed by facile cyclization and hydrogen shift prior to hydrogen atom emission and aromatization to racemic mixtures (ortho, meta) of biphenyls in overall exoergic reactions. These findings not only challenge our current perception of biphenyls as high temperature markers in combustion systems and astrophysical environments, but also identify biphenyls as fundamental building blocks of complex polycyclic aromatic hydrocarbons (PAHs) such as coronene (C24H12) eventually leading to carbonaceous nanoparticles (soot, grains) in combustion systems and in deep space thus affording critical insight into the low-temperature hydrocarbon chemistry in our universe.
{"title":"Unconventional gas-phase synthesis of biphenyl and its atropisomeric methyl-substituted derivatives.","authors":"Shane J Goettl, Chao He, Zhenghai Yang, Ralf I Kaiser, Ankit Somani, Adrian Portela-Gonzalez, Wolfram Sander, Bing-Jian Sun, Siti Fatimah, Komal P Kadam, Agnes H H Chang","doi":"10.1039/d4cp00765d","DOIUrl":"10.1039/d4cp00765d","url":null,"abstract":"<p><p>The biphenyl molecule (C<sub>12</sub>H<sub>10</sub>) acts as a fundamental molecular backbone in the stereoselective synthesis of organic materials due to its inherent twist angle causing atropisomerism in substituted derivatives and in molecular mass growth processes in circumstellar environments and combustion systems. Here, we reveal an unconventional low-temperature phenylethynyl addition-cyclization-aromatization mechanism for the gas-phase preparation of biphenyl (C<sub>12</sub>H<sub>10</sub>) along with <i>ortho</i>-, <i>meta</i>-, and <i>para</i>-substituted methylbiphenyl (C<sub>13</sub>H<sub>12</sub>) derivatives through crossed molecular beams and computational studies providing compelling evidence on their formation <i>via</i> bimolecular gas-phase reactions of phenylethynyl radicals (C<sub>6</sub>H<sub>5</sub>CC, X<sup>2</sup>A<sub>1</sub>) with 1,3-butadiene-<i>d</i><sub>6</sub> (C<sub>4</sub>D<sub>6</sub>), isoprene (CH<sub>2</sub>C(CH<sub>3</sub>)CHCH<sub>2</sub>), and 1,3-pentadiene (CH<sub>2</sub>CHCHCHCH<sub>3</sub>). The dynamics involve de-facto barrierless phenylethynyl radical additions <i>via</i> submerged barriers followed by facile cyclization and hydrogen shift prior to hydrogen atom emission and aromatization to racemic mixtures (<i>ortho</i>, <i>meta</i>) of biphenyls in overall exoergic reactions. These findings not only challenge our current perception of biphenyls as high temperature markers in combustion systems and astrophysical environments, but also identify biphenyls as fundamental building blocks of complex polycyclic aromatic hydrocarbons (PAHs) such as coronene (C<sub>24</sub>H<sub>12</sub>) eventually leading to carbonaceous nanoparticles (soot, grains) in combustion systems and in deep space thus affording critical insight into the low-temperature hydrocarbon chemistry in our universe.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":null,"pages":null},"PeriodicalIF":2.9,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141441853","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Thi Luu Luyen Doan, Minh Xuan Tran, Dang Le Tri Nguyen, Dinh Chuong Nguyen
In this study, we developed a high-performance non-enzymatic electrochemical sensor based on urchin-like CoP3/Cu3P heterostructured nanorods supported on a three-dimensional porous copper foam, namely, CoP3/Cu3P NRs/CF, for the detection of dopamine. Benefiting from the promising intrinsic catalytic activities of CoP3 and Cu3P, urchin-like microsphere structures, and a large electrochemically active surface area for exposing numerous accessible catalytic active sites, the proposed CoP3/Cu3P NRs/CF shows extraordinary electrochemical response towards the electrocatalytic oxidation of dopamine. As a result, the CoP3/Cu3P NRs/CF sensing electrode has a broad detection window (from 0.2 to 2000 μM), low detection limit (0.51 μM), high electrochemical sensitivity (0.0105 mA μM-1 cm-2), excellent selectivity towards dopamine in the coexistence of some interfering species, and good stability for dopamine determination. More importantly, the CoP3/Cu3P NRs/CF catalyst also exhibits excellent catalytic activity, sensitivity, and selectivity for dopamine detection under simulated human body conditions at a physiological pH of 7.25 (0.1 M PBS) at 36.6 °C.
{"title":"Urchin-like CoP<sub>3</sub>/Cu<sub>3</sub>P heterostructured nanorods supported on a 3D porous copper foam for high-performance non-enzymatic electrochemical dopamine sensors.","authors":"Thi Luu Luyen Doan, Minh Xuan Tran, Dang Le Tri Nguyen, Dinh Chuong Nguyen","doi":"10.1039/d3cp04340a","DOIUrl":"10.1039/d3cp04340a","url":null,"abstract":"<p><p>In this study, we developed a high-performance non-enzymatic electrochemical sensor based on urchin-like CoP<sub>3</sub>/Cu<sub>3</sub>P heterostructured nanorods supported on a three-dimensional porous copper foam, namely, CoP<sub>3</sub>/Cu<sub>3</sub>P NRs/CF, for the detection of dopamine. Benefiting from the promising intrinsic catalytic activities of CoP<sub>3</sub> and Cu<sub>3</sub>P, urchin-like microsphere structures, and a large electrochemically active surface area for exposing numerous accessible catalytic active sites, the proposed CoP<sub>3</sub>/Cu<sub>3</sub>P NRs/CF shows extraordinary electrochemical response towards the electrocatalytic oxidation of dopamine. As a result, the CoP<sub>3</sub>/Cu<sub>3</sub>P NRs/CF sensing electrode has a broad detection window (from 0.2 to 2000 μM), low detection limit (0.51 μM), high electrochemical sensitivity (0.0105 mA μM<sup>-1</sup> cm<sup>-2</sup>), excellent selectivity towards dopamine in the coexistence of some interfering species, and good stability for dopamine determination. More importantly, the CoP<sub>3</sub>/Cu<sub>3</sub>P NRs/CF catalyst also exhibits excellent catalytic activity, sensitivity, and selectivity for dopamine detection under simulated human body conditions at a physiological pH of 7.25 (0.1 M PBS) at 36.6 °C.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":null,"pages":null},"PeriodicalIF":2.9,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141445631","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Hyun-Sik Kim, Nicholas A Heinz, Zachary M Gibbs, Junsu Kim, G Jeffrey Snyder
Nanostructured thermoelectric materials ideally reduce lattice thermal conductivity without harming the electrical properties. Thus, to truly improve the thermoelectric performance, the quality factor, which is proportional to the weighted mobility divided by the lattice thermal conductivity of the material, must be improved. Precipitates of In2Te3 form in the state-of-the-art Bi2Te3 with crystallographic alignment to the Bi2Te3 structure. Like epitaxy in films, this can be called endotaxy in solids. This natural epitaxy in a 3-dimensional solid is ideally situated to scatter phonons but produces minimal electronic scattering and, therefore, maintains high mobility. Here, we study the effects of In-alloying in Bi2Te3 at high In concentrations (about 4 at%), enough to produce the endotaxial microstructure. It is found that such concentrations of indium in Bi2Te3 significantly alter the electronic structure, reducing the effective mass and weighted mobility so significantly as to effectively destroy the thermoelectric properties even though the lattice thermal conductivity is successfully reduced.
{"title":"Transport properties of indium-alloyed and indium telluride nanostructured bismuth telluride.","authors":"Hyun-Sik Kim, Nicholas A Heinz, Zachary M Gibbs, Junsu Kim, G Jeffrey Snyder","doi":"10.1039/d4cp01296h","DOIUrl":"10.1039/d4cp01296h","url":null,"abstract":"<p><p>Nanostructured thermoelectric materials ideally reduce lattice thermal conductivity without harming the electrical properties. Thus, to truly improve the thermoelectric performance, the quality factor, which is proportional to the weighted mobility divided by the lattice thermal conductivity of the material, must be improved. Precipitates of In<sub>2</sub>Te<sub>3</sub> form in the state-of-the-art Bi<sub>2</sub>Te<sub>3</sub> with crystallographic alignment to the Bi<sub>2</sub>Te<sub>3</sub> structure. Like epitaxy in films, this can be called endotaxy in solids. This natural epitaxy in a 3-dimensional solid is ideally situated to scatter phonons but produces minimal electronic scattering and, therefore, maintains high mobility. Here, we study the effects of In-alloying in Bi<sub>2</sub>Te<sub>3</sub> at high In concentrations (about 4 at%), enough to produce the endotaxial microstructure. It is found that such concentrations of indium in Bi<sub>2</sub>Te<sub>3</sub> significantly alter the electronic structure, reducing the effective mass and weighted mobility so significantly as to effectively destroy the thermoelectric properties even though the lattice thermal conductivity is successfully reduced.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":null,"pages":null},"PeriodicalIF":2.9,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141416762","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}