Rafael Flores-Larrañaga, María Eugenia Castro, Alejandro Palma, Francisco J. Melendez
Benzophenone is a molecule with several extremely relevant characteristics, widely used as a type-2 photoinitiator due to its unique electronic properties and a very efficient intersystem crossing. In general, benzophenone can absorb directly to S1 or S2 states, but S0 → S1 transition is weak. Also, benzophenone has symmetric activity of the torsional modes of the phenyl groups, suggesting that is a non-rigid molecule. This work has two fundamental purposes. The first is to examine the ground state (S0) and first singlet excited state (S1) of benzophenone using TD-DFT methodology to generate the potential energy surface (PES) to understand its non-rigid behavior; and the second, to examine the Franck-Condon factors (FC factors) between the transition S0 → S1. From our results, the most accurate was the hybrid functional PBE0. From the PES analysis of S0 and S1 states, we observe that several minima were located and that they are separated by relative low energy barriers. The global minimum of S0 is found at θ1/θ2 = 28.15° and for S1 at θ1/θ2 = 20.71°. Interestingly, the PES of S1 state shows a very extensive area of minimum energy and a local minimum located at θ1 = 90.71°/θ2 = 0.71°. From the vibrational spectra, we observe two intense signals that correspond to the symmetric phenyl twisting of normal mode 2 (23 and 24), and a combination between the symmetric hydrogen scissoring of 441 and 23. As the vibronic spectrum tells, this transition is forbidden by the orbital theory but it is electronically allowed. Also, from the Duschinksy matrix, we observe a high mixing of vibrational modes.
{"title":"Theoretical Insights of the Non-Rigid Behavior of Benzophenone by Franck-Condon Factors Approach","authors":"Rafael Flores-Larrañaga, María Eugenia Castro, Alejandro Palma, Francisco J. Melendez","doi":"10.1002/qua.70019","DOIUrl":"https://doi.org/10.1002/qua.70019","url":null,"abstract":"<div>\u0000 \u0000 <p>Benzophenone is a molecule with several extremely relevant characteristics, widely used as a type-2 photoinitiator due to its unique electronic properties and a very efficient intersystem crossing. In general, benzophenone can absorb directly to S<sub>1</sub> or S<sub>2</sub> states, but S<sub>0</sub> → S<sub>1</sub> transition is weak. Also, benzophenone has symmetric activity of the torsional modes of the phenyl groups, suggesting that is a non-rigid molecule. This work has two fundamental purposes. The first is to examine the ground state (S<sub>0</sub>) and first singlet excited state (S<sub>1</sub>) of benzophenone using TD-DFT methodology to generate the potential energy surface (PES) to understand its non-rigid behavior; and the second, to examine the Franck-Condon factors (FC factors) between the transition S<sub>0</sub> → S<sub>1</sub>. From our results, the most accurate was the hybrid functional PBE0. From the PES analysis of S<sub>0</sub> and S<sub>1</sub> states, we observe that several minima were located and that they are separated by relative low energy barriers. The global minimum of S<sub>0</sub> is found at <i>θ</i><sub>1</sub>/<i>θ</i><sub>2</sub> = 28.15° and for S<sub>1</sub> at <i>θ</i><sub>1</sub>/<i>θ</i><sub>2</sub> = 20.71°. Interestingly, the PES of S<sub>1</sub> state shows a very extensive area of minimum energy and a local minimum located at <i>θ</i><sub>1</sub> = 90.71°/<i>θ</i><sub>2</sub> = 0.71°. From the vibrational spectra, we observe two intense signals that correspond to the symmetric phenyl twisting of normal mode 2 (2<sup>3</sup> and 2<sup>4</sup>), and a combination between the symmetric hydrogen scissoring of 44<sup>1</sup> and 2<sup>3</sup>. As the vibronic spectrum tells, this transition is forbidden by the orbital theory but it is electronically allowed. Also, from the Duschinksy matrix, we observe a high mixing of vibrational modes.</p>\u0000 </div>","PeriodicalId":182,"journal":{"name":"International Journal of Quantum Chemistry","volume":"125 4","pages":""},"PeriodicalIF":2.3,"publicationDate":"2025-02-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143389023","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}
Md. Bayjid Hossain Parosh, Mohshina Binte Mansur, Nusrat Jahan Nisha, Istiak Ahmed Ovi, Md. Jahirul Islam, Jehan Y. Al-Humaidi, Md. Rasidul Islam
Comparative exploration of structural, population analysis, mechanical, electronic, optical, and magnetic properties of a zinc-based single, non-toxic, inorganic halide-based novel perovskite compound RbZnX3 (X = F, Cl, and Br) without applying pressure by using GGA-PBE functional within the CASTEP code. Systematic investigations show mechanically stable compound with lattice parameters of the unit cell 4.25, 5.01, 5.50 Å, with indirect bandgaps of 3.637, 1.387, 0.103 eV for RbZnF3, RbZnCl3, and RbZnBr3 respectively. Band gap data shows that RbZnX3 is a semiconductor in nature, and RbZnCl3 can be an ideal photovoltaic material. From CDD analysis, all three perovskites show a combination of metallic and ionic bonding. Computed optical properties ensure this compound is beneficial in PES and EUV-based applications, like- anti-reflection surface coating and optoelectronics like solar cells, and it can be a promising element in radiation shielding, spectroscopy, and biotech fields, as well as in high absorption and infrared sectors. High reflectivity makes them suitable as solar cell coating material. Mechanical properties ensure these studied elements' ductility, machinability, and anisotropy. Absorption and reflectivity diminish where energy loss is maximum. For being diamagnetic, it is for superconductors, electromagnetic shielding, and materials testing sectors. Moreover, this study focuses on various applications and possibilities of this compound. Materials are found ductile and RbZnF3 has an excellent shear and bulk modulus. RbZnF3 exhibits more significant fracture and plastic deformation resistance than RbZnCl3 and RbZnBr3. Moderate elasticity, flexibility, and strength make these suitable for various applications. The phonon calculation indicates that RbZnF3 exhibits dynamic stability, whereas instability has been observed in RbZnCl3 and RbZnBr3. An increase in Debye temperature correlates with improved elastic modulus, elevated sound velocity, and higher melting temperature. RbZnBr3 shows higher heat capacity at (T < < θD) and shows higher energy dispersion or entropy.
{"title":"DFT Investigations of Non-Toxic Perovskites RbZnX3 (X = F, Cl, and Br): Analyzing the Structural, Electrical, Optical, Mechanical, and Thermodynamic Properties for Suitable Optoelectronic Applications","authors":"Md. Bayjid Hossain Parosh, Mohshina Binte Mansur, Nusrat Jahan Nisha, Istiak Ahmed Ovi, Md. Jahirul Islam, Jehan Y. Al-Humaidi, Md. Rasidul Islam","doi":"10.1002/qua.70014","DOIUrl":"https://doi.org/10.1002/qua.70014","url":null,"abstract":"<div>\u0000 \u0000 <p>Comparative exploration of structural, population analysis, mechanical, electronic, optical, and magnetic properties of a zinc-based single, non-toxic, inorganic halide-based novel perovskite compound RbZnX<sub>3</sub> (X = F, Cl, and Br) without applying pressure by using GGA-PBE functional within the CASTEP code. Systematic investigations show mechanically stable compound with lattice parameters of the unit cell 4.25, 5.01, 5.50 Å, with indirect bandgaps of 3.637, 1.387, 0.103 eV for RbZnF<sub>3</sub>, RbZnCl<sub>3</sub>, and RbZnBr<sub>3</sub> respectively. Band gap data shows that RbZnX<sub>3</sub> is a semiconductor in nature, and RbZnCl<sub>3</sub> can be an ideal photovoltaic material. From CDD analysis, all three perovskites show a combination of metallic and ionic bonding. Computed optical properties ensure this compound is beneficial in PES and EUV-based applications, like- anti-reflection surface coating and optoelectronics like solar cells, and it can be a promising element in radiation shielding, spectroscopy, and biotech fields, as well as in high absorption and infrared sectors. High reflectivity makes them suitable as solar cell coating material. Mechanical properties ensure these studied elements' ductility, machinability, and anisotropy. Absorption and reflectivity diminish where energy loss is maximum. For being diamagnetic, it is for superconductors, electromagnetic shielding, and materials testing sectors. Moreover, this study focuses on various applications and possibilities of this compound. Materials are found ductile and RbZnF<sub>3</sub> has an excellent shear and bulk modulus. RbZnF<sub>3</sub> exhibits more significant fracture and plastic deformation resistance than RbZnCl<sub>3</sub> and RbZnBr<sub>3</sub>. Moderate elasticity, flexibility, and strength make these suitable for various applications. The phonon calculation indicates that RbZnF<sub>3</sub> exhibits dynamic stability, whereas instability has been observed in RbZnCl<sub>3</sub> and RbZnBr<sub>3</sub>. An increase in Debye temperature correlates with improved elastic modulus, elevated sound velocity, and higher melting temperature. RbZnBr<sub>3</sub> shows higher heat capacity at (<i>T</i> < < <i>θ</i><sub>D</sub>) and shows higher energy dispersion or entropy.</p>\u0000 </div>","PeriodicalId":182,"journal":{"name":"International Journal of Quantum Chemistry","volume":"125 4","pages":""},"PeriodicalIF":2.3,"publicationDate":"2025-02-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143380142","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}
Chaoyong Wang, Gan Yong, Yanbin Li, Fuhao Qi, Hanyu Du, Jun Zhao, Junji Guo, Kai Wang
In this work, the structures and electronic properties of anionic, neutral, and cationic TMPb16−/0/+ (TM = Sc, Y, Ti, Zr, Hf) clusters were studied through a genetic algorithm (GA) code with density functional theory (DFT) calculations. The results show that anionic TMPb16− (TM = Sc, Y, Ti, Zr) and neutral TMPb16 (TM = Ti, Zr, Hf) clusters adopt the Frank–Kasper (FK) polyhedron as the geometric structure, while TMPb16 (TM = Sc, Y, Hf−) and all cationic states of these clusters prefer a fullerene-like bitruncated square trapezohedron. In these clusters, the gain and loss of electrons in transition metals (TM) are similar and very small, with only Hf atom as the electron donor. The average binding energy of cationic TMPb16 is 0.02 and 0.1 eV higher than that of its anionic and neutral states, respectively. All these TMPb16 (TM = Sc−, Y−, Ti, Zr, Hf) clusters with 68 electrons show superatomic features with the electronic shell configuration of (1S)2(1P)6(1D)10(1F)14(2S)2(1G)18(2P)6(2D)10 as same as that of TMSn16 (TM = Sc−, Y−, Ti, Zr, Hf) clusters.
{"title":"Structures and Electronic Properties of TMPb16−/0/+ (TM = Sc, Y, Ti, Zr, Hf) Clusters","authors":"Chaoyong Wang, Gan Yong, Yanbin Li, Fuhao Qi, Hanyu Du, Jun Zhao, Junji Guo, Kai Wang","doi":"10.1002/qua.70016","DOIUrl":"https://doi.org/10.1002/qua.70016","url":null,"abstract":"<div>\u0000 \u0000 <p>In this work, the structures and electronic properties of anionic, neutral, and cationic TMPb<sub>16</sub><sup>−/0/+</sup> (TM = Sc, Y, Ti, Zr, Hf) clusters were studied through a genetic algorithm (GA) code with density functional theory (DFT) calculations. The results show that anionic TMPb<sub>16</sub><sup>−</sup> (TM = Sc, Y, Ti, Zr) and neutral TMPb<sub>16</sub> (TM = Ti, Zr, Hf) clusters adopt the Frank–Kasper (FK) polyhedron as the geometric structure, while TMPb<sub>16</sub> (TM = Sc, Y, Hf<sup>−</sup>) and all cationic states of these clusters prefer a fullerene-like bitruncated square trapezohedron. In these clusters, the gain and loss of electrons in transition metals (TM) are similar and very small, with only Hf atom as the electron donor. The average binding energy of cationic TMPb<sub>16</sub> is 0.02 and 0.1 eV higher than that of its anionic and neutral states, respectively. All these TMPb<sub>16</sub> (TM = Sc<sup>−</sup>, Y<sup>−</sup>, Ti, Zr, Hf) clusters with 68 electrons show superatomic features with the electronic shell configuration of (1S)<sup>2</sup>(1P)<sup>6</sup>(1D)<sup>10</sup>(1F)<sup>14</sup>(2S)<sup>2</sup>(1G)<sup>18</sup>(2P)<sup>6</sup>(2D)<sup>10</sup> as same as that of TMSn<sub>16</sub> (TM = Sc<sup>−</sup>, Y<sup>−</sup>, Ti, Zr, Hf) clusters.</p>\u0000 </div>","PeriodicalId":182,"journal":{"name":"International Journal of Quantum Chemistry","volume":"125 4","pages":""},"PeriodicalIF":2.3,"publicationDate":"2025-02-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143370081","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}
Maliheh Shaban Tameh, Wayne L. Gladfelter, Jason D. Goodpaster
<p>The ability of SnO<sub>2</sub> surfaces to adsorb and activate oxygen species is essential for designing high-performance gas sensors and catalytic materials. In this study, density functional theory (DFT) calculations are employed to unravel the mechanisms governing oxygen adsorption on SnO<sub>2</sub> (110) surfaces under varying surface conditions, including reduced, defective, and stoichiometric configurations. Our findings indicate various forms of charged oxygen species on the surface. The study reveals the presence of <span></span><math> <semantics> <mrow> <msubsup> <mi>O</mi> <mn>2</mn> <mrow> <mn>2</mn> <mo>−</mo> </mrow> </msubsup> </mrow> <annotation>$$ {mathrm{O}}_2^{2-} $$</annotation> </semantics></math>, <span></span><math> <semantics> <mrow> <msubsup> <mi>O</mi> <mn>2</mn> <mo>−</mo> </msubsup> </mrow> <annotation>$$ {mathrm{O}}_2^{-} $$</annotation> </semantics></math>, and <span></span><math> <semantics> <mrow> <msup> <mi>O</mi> <mrow> <mn>2</mn> <mo>−</mo> </mrow> </msup> </mrow> <annotation>$$ {mathrm{O}}^{2-} $$</annotation> </semantics></math> on the reduced surface and <span></span><math> <semantics> <mrow> <msubsup> <mi>O</mi> <mn>2</mn> <mrow> <mn>2</mn> <mo>−</mo> </mrow> </msubsup> </mrow> <annotation>$$ {mathrm{O}}_2^{2-} $$</annotation> </semantics></math>, <span></span><math> <semantics> <mrow> <msup> <mi>O</mi> <mo>−</mo> </msup> </mrow> <annotation>$$ {mathrm{O}}^{-} $$</annotation> </semantics></math>, and <span></span><math> <semantics> <mrow> <msup> <mi>O</mi> <mrow> <mn>2</mn> <mo>−</mo> </mrow> </msup> </mrow> <annotation
{"title":"Unraveling Surface Chemistry of SnO2 Through Formation of Charged Oxygen Species and Oxygen Vacancies","authors":"Maliheh Shaban Tameh, Wayne L. Gladfelter, Jason D. Goodpaster","doi":"10.1002/qua.70017","DOIUrl":"https://doi.org/10.1002/qua.70017","url":null,"abstract":"<p>The ability of SnO<sub>2</sub> surfaces to adsorb and activate oxygen species is essential for designing high-performance gas sensors and catalytic materials. In this study, density functional theory (DFT) calculations are employed to unravel the mechanisms governing oxygen adsorption on SnO<sub>2</sub> (110) surfaces under varying surface conditions, including reduced, defective, and stoichiometric configurations. Our findings indicate various forms of charged oxygen species on the surface. The study reveals the presence of <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <msubsup>\u0000 <mi>O</mi>\u0000 <mn>2</mn>\u0000 <mrow>\u0000 <mn>2</mn>\u0000 <mo>−</mo>\u0000 </mrow>\u0000 </msubsup>\u0000 </mrow>\u0000 <annotation>$$ {mathrm{O}}_2^{2-} $$</annotation>\u0000 </semantics></math>, <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <msubsup>\u0000 <mi>O</mi>\u0000 <mn>2</mn>\u0000 <mo>−</mo>\u0000 </msubsup>\u0000 </mrow>\u0000 <annotation>$$ {mathrm{O}}_2^{-} $$</annotation>\u0000 </semantics></math>, and <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <msup>\u0000 <mi>O</mi>\u0000 <mrow>\u0000 <mn>2</mn>\u0000 <mo>−</mo>\u0000 </mrow>\u0000 </msup>\u0000 </mrow>\u0000 <annotation>$$ {mathrm{O}}^{2-} $$</annotation>\u0000 </semantics></math> on the reduced surface and <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <msubsup>\u0000 <mi>O</mi>\u0000 <mn>2</mn>\u0000 <mrow>\u0000 <mn>2</mn>\u0000 <mo>−</mo>\u0000 </mrow>\u0000 </msubsup>\u0000 </mrow>\u0000 <annotation>$$ {mathrm{O}}_2^{2-} $$</annotation>\u0000 </semantics></math>, <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <msup>\u0000 <mi>O</mi>\u0000 <mo>−</mo>\u0000 </msup>\u0000 </mrow>\u0000 <annotation>$$ {mathrm{O}}^{-} $$</annotation>\u0000 </semantics></math>, and <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <msup>\u0000 <mi>O</mi>\u0000 <mrow>\u0000 <mn>2</mn>\u0000 <mo>−</mo>\u0000 </mrow>\u0000 </msup>\u0000 </mrow>\u0000 <annotation","PeriodicalId":182,"journal":{"name":"International Journal of Quantum Chemistry","volume":"125 4","pages":""},"PeriodicalIF":2.3,"publicationDate":"2025-02-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/qua.70017","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143362940","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
A. Dixit, A. Saxena, J.A. Abraham, S. Dubey, R. Sharma, S.M.H. Qaid, I. Štich, M. Aslam, and A. Zetsepin, “Hydrostatic Pressure-Tuning of Opto-Electronic and Thermoelectric Properties Half-Heusler Alloy RhTiP With DFT Analysis,” International Journal of Quantum Chemistry, 124 (2024): e27482, https://doi.org/10.1002/qua.27482.
The author affiliation for Saif M. H. Qaid originally published without including the correct information. The affiliation should have been as follows:
6Department of Physics & Astronomy, College of Science, King Saud University, Riyadh, Saudi Arabia.
In addition, the King Saud University funding information had the wrong identification number and should have been as follows:
Funding: This research was supported by King Saud University (RSPD2024R762).
We apologize for the error.
{"title":"Correction to Hydrostatic Pressure-Tuning of Opto-Electronic and Thermoelectric Properties Half-Heusler Alloy RhTiP With DFT Analysis","authors":"","doi":"10.1002/qua.70010","DOIUrl":"https://doi.org/10.1002/qua.70010","url":null,"abstract":"<p>A. Dixit, A. Saxena, J.A. Abraham, S. Dubey, R. Sharma, S.M.H. Qaid, I. Štich, M. Aslam, and A. Zetsepin, “Hydrostatic Pressure-Tuning of Opto-Electronic and Thermoelectric Properties Half-Heusler Alloy RhTiP With DFT Analysis,” <i>International Journal of Quantum Chemistry</i>, 124 (2024): e27482, https://doi.org/10.1002/qua.27482.</p><p>The author affiliation for Saif M. H. Qaid originally published without including the correct information. The affiliation should have been as follows:</p><p><sup>6</sup>Department of Physics & Astronomy, College of Science, King Saud University, Riyadh, Saudi Arabia.</p><p>In addition, the King Saud University funding information had the wrong identification number and should have been as follows:</p><p><b>Funding:</b> This research was supported by King Saud University (RSPD2024R762).</p><p>We apologize for the error.</p>","PeriodicalId":182,"journal":{"name":"International Journal of Quantum Chemistry","volume":"125 3","pages":""},"PeriodicalIF":2.3,"publicationDate":"2025-02-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/qua.70010","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143111568","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Polytetrafluoroethylene (PTFE) is widely used in fields such as propellants and flame retardants. However, this is still a vacancy of detailed kinetic mechanisms to describe the complete decomposition of PTFE in the gas phase. The current work addresses this issue by conducting ab initio calculations for key reactions involved in the PTFE pyrolysis system. The potential energy surfaces (PESs) of PTFE unimolecular and bimolecular reactions are determined at the DLPNO-CCSD(T)/cc-pVTZ//B3LYP-D3/6–31++G(d,p) level. Rate constants and branching ratios of the main reaction pathways are calculated by solving the RRKM master equation, and the thermochemical properties of related species at the DLPNO-CCSD(T)/CBS level are calculated via the atomization method. The current study found that the initial decomposition of PTFE is dominated by the CC scission reactions and free radical (H, OH, CF, CF2, and CF3) abstraction reactions, forming the corresponding free radical species. Further β-CC scission reactions dominate the overall kinetics and continuously generate CF2CF2. Self-decomposition and free radical–driven decomposition of PTFE produce small molecules such as HF, FOH, CF2, CF3, and CF4. This work provides quantitative predictions of the detailed decomposition reaction pathways of gas-phase PTFE and will lay a solid foundation for the development of detailed kinetic mechanisms for PTFE combustion and degradation.
{"title":"Pyrolysis Kinetics of Polytetrafluoroethylene (PTFE)","authors":"Yongjin Wang, Shengkai Wang, Qingzhao Chu, Dongping Chen","doi":"10.1002/qua.70015","DOIUrl":"https://doi.org/10.1002/qua.70015","url":null,"abstract":"<div>\u0000 \u0000 <p>Polytetrafluoroethylene (PTFE) is widely used in fields such as propellants and flame retardants. However, this is still a vacancy of detailed kinetic mechanisms to describe the complete decomposition of PTFE in the gas phase. The current work addresses this issue by conducting ab initio calculations for key reactions involved in the PTFE pyrolysis system. The potential energy surfaces (PESs) of PTFE unimolecular and bimolecular reactions are determined at the DLPNO-CCSD(T)/cc-pVTZ//B3LYP-D3/6–31++G(d,p) level. Rate constants and branching ratios of the main reaction pathways are calculated by solving the RRKM master equation, and the thermochemical properties of related species at the DLPNO-CCSD(T)/CBS level are calculated via the atomization method. The current study found that the initial decomposition of PTFE is dominated by the C<span></span>C scission reactions and free radical (H, OH, CF, CF<sub>2</sub>, and CF<sub>3</sub>) abstraction reactions, forming the corresponding free radical species. Further β-C<span></span>C scission reactions dominate the overall kinetics and continuously generate CF<sub>2</sub>CF<sub>2</sub>. Self-decomposition and free radical–driven decomposition of PTFE produce small molecules such as HF, FOH, CF<sub>2</sub>, CF<sub>3</sub>, and CF<sub>4</sub>. This work provides quantitative predictions of the detailed decomposition reaction pathways of gas-phase PTFE and will lay a solid foundation for the development of detailed kinetic mechanisms for PTFE combustion and degradation.</p>\u0000 </div>","PeriodicalId":182,"journal":{"name":"International Journal of Quantum Chemistry","volume":"125 3","pages":""},"PeriodicalIF":2.3,"publicationDate":"2025-02-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143111163","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}
<p> <span>B. Nagy</span>, “ <span>The Hyper-Wiener Index of Diamond Nanowires</span>,” <i>International Journal of Quantum Chemistry</i> <span>124</span>, no. <span>1</span> (<span>2024</span>): e27258.</p><p>There is a miscalculation in the above paper; the correct formula and value of hyper-Wiener indices are presented here. The numbering is from the original article; the correct versions of the equations with the corrected proof can be found below.</p><p>Now we state our main results.</p><p> </p><p> </p><p> </p><p>Some of the first elements of the sequence defined above give the hyper-Wiener index of relatively small diamond grid samples, that is, <span></span><math> <semantics> <mrow> <mi>W</mi> <mi>W</mi> <mo>(</mo> <msub> <mrow> <mi>G</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> <mo>)</mo> <mo>=</mo> <mn>460</mn> </mrow> <annotation>$$ WWleft({G}_1right)=460 $$</annotation> </semantics></math>, <span></span><math> <semantics> <mrow> <mi>W</mi> <mi>W</mi> <mo>(</mo> <msub> <mrow> <mi>G</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> <mo>)</mo> <mo>=</mo> <mn>3556</mn> </mrow> <annotation>$$ WWleft({G}_2right)=3556 $$</annotation> </semantics></math>, <span></span><math> <semantics> <mrow> <mi>W</mi> <mi>W</mi> <mo>(</mo> <msub> <mrow> <mi>G</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> <mo>)</mo> <mo>=</mo> <mn>14</mn> <mspace></mspace> <mn>306</mn> </mrow> <annotation>$$ WWleft({G}_3right)=14kern0.2em 306 $$</annotation> </semantics></math>, <span></span><math> <semantics> <mrow> <mi>W</mi> <mi>W</mi> <mo>(</mo> <msub> <mrow>
{"title":"Correction to “The hyper-Wiener index of diamond nanowires”","authors":"","doi":"10.1002/qua.27514","DOIUrl":"https://doi.org/10.1002/qua.27514","url":null,"abstract":"<p>\u0000 <span>B. Nagy</span>, “ <span>The Hyper-Wiener Index of Diamond Nanowires</span>,” <i>International Journal of Quantum Chemistry</i> <span>124</span>, no. <span>1</span> (<span>2024</span>): e27258.</p><p>There is a miscalculation in the above paper; the correct formula and value of hyper-Wiener indices are presented here. The numbering is from the original article; the correct versions of the equations with the corrected proof can be found below.</p><p>Now we state our main results.</p><p>\u0000 </p><p>\u0000 </p><p>\u0000 </p><p>Some of the first elements of the sequence defined above give the hyper-Wiener index of relatively small diamond grid samples, that is, <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <mi>W</mi>\u0000 <mi>W</mi>\u0000 <mo>(</mo>\u0000 <msub>\u0000 <mrow>\u0000 <mi>G</mi>\u0000 </mrow>\u0000 <mrow>\u0000 <mn>1</mn>\u0000 </mrow>\u0000 </msub>\u0000 <mo>)</mo>\u0000 <mo>=</mo>\u0000 <mn>460</mn>\u0000 </mrow>\u0000 <annotation>$$ WWleft({G}_1right)=460 $$</annotation>\u0000 </semantics></math>, <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <mi>W</mi>\u0000 <mi>W</mi>\u0000 <mo>(</mo>\u0000 <msub>\u0000 <mrow>\u0000 <mi>G</mi>\u0000 </mrow>\u0000 <mrow>\u0000 <mn>2</mn>\u0000 </mrow>\u0000 </msub>\u0000 <mo>)</mo>\u0000 <mo>=</mo>\u0000 <mn>3556</mn>\u0000 </mrow>\u0000 <annotation>$$ WWleft({G}_2right)=3556 $$</annotation>\u0000 </semantics></math>, <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <mi>W</mi>\u0000 <mi>W</mi>\u0000 <mo>(</mo>\u0000 <msub>\u0000 <mrow>\u0000 <mi>G</mi>\u0000 </mrow>\u0000 <mrow>\u0000 <mn>3</mn>\u0000 </mrow>\u0000 </msub>\u0000 <mo>)</mo>\u0000 <mo>=</mo>\u0000 <mn>14</mn>\u0000 <mspace></mspace>\u0000 <mn>306</mn>\u0000 </mrow>\u0000 <annotation>$$ WWleft({G}_3right)=14kern0.2em 306 $$</annotation>\u0000 </semantics></math>, <span></span><math>\u0000 <semantics>\u0000 <mrow>\u0000 <mi>W</mi>\u0000 <mi>W</mi>\u0000 <mo>(</mo>\u0000 <msub>\u0000 <mrow>\u0000 ","PeriodicalId":182,"journal":{"name":"International Journal of Quantum Chemistry","volume":"125 3","pages":""},"PeriodicalIF":2.3,"publicationDate":"2025-01-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/qua.27514","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143110477","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Tahira Bashir, Khalid M. Alotaibi, Sajad Ali, Hayat Ullah, Kashif Safeen, Akif Safeen, Immad-Uddin, Yousuf Iqbal, Syed Taj Ud Din
This study employs first-principles computations to analyze ferrite spinels GeFe2O4 and SmFe2O4 using density functional theory (DFT). Structural stability calculations reveal that GeFe2O4 favors an antiferromagnetic phase, while SmFe2O4 stabilizes in a ferrimagnetic phase. Both compounds are elastically stable and ductile, and exhibit lattice constants consistent with experimental values, validating the reliability of the calculations. A significant drop in Debye temperature (from 495 to 233 K) occurs when Ge is replaced by Sm, while high melting temperatures indicate thermal stability over broad temperature ranges. The spin-polarized electronic band structure confirms the metallic nature of both materials. Furthermore, the Curie temperature and magnetic moment of SmFe2O4, calculated using Generalized Gradient Approximation (GGA + U) and the Heyd–Scuseria–Ernzerhof (HSE) methods, underline its potential for spintronic applications.
{"title":"Investigation of the Structural, Mechanical, Thermal, and Magneto-Electronic Properties of Promising Ferrite Spinel Oxides XFe2O4 (X = Ge and Sm): A First-Principle Approach","authors":"Tahira Bashir, Khalid M. Alotaibi, Sajad Ali, Hayat Ullah, Kashif Safeen, Akif Safeen, Immad-Uddin, Yousuf Iqbal, Syed Taj Ud Din","doi":"10.1002/qua.70009","DOIUrl":"https://doi.org/10.1002/qua.70009","url":null,"abstract":"<div>\u0000 \u0000 <p>This study employs first-principles computations to analyze ferrite spinels GeFe<sub>2</sub>O<sub>4</sub> and SmFe<sub>2</sub>O<sub>4</sub> using density functional theory (DFT). Structural stability calculations reveal that GeFe<sub>2</sub>O<sub>4</sub> favors an antiferromagnetic phase, while SmFe<sub>2</sub>O<sub>4</sub> stabilizes in a ferrimagnetic phase. Both compounds are elastically stable and ductile, and exhibit lattice constants consistent with experimental values, validating the reliability of the calculations. A significant drop in Debye temperature (from 495 to 233 K) occurs when Ge is replaced by Sm, while high melting temperatures indicate thermal stability over broad temperature ranges. The spin-polarized electronic band structure confirms the metallic nature of both materials. Furthermore, the Curie temperature and magnetic moment of SmFe<sub>2</sub>O<sub>4</sub>, calculated using Generalized Gradient Approximation (GGA + U) and the Heyd–Scuseria–Ernzerhof (HSE) methods, underline its potential for spintronic applications.</p>\u0000 </div>","PeriodicalId":182,"journal":{"name":"International Journal of Quantum Chemistry","volume":"125 3","pages":""},"PeriodicalIF":2.3,"publicationDate":"2025-01-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143118780","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}
Xin Wei, Fengjun Liu, Mengyu Zhu, Lin Wang, Maolin Sha
We systematically explored the adsorption, diffusion, thermodynamics stability, and electrochemical performance of halogen anions (F−, Cl−, Br−, I−) on monolayer InSe using first-principles calculations. F−, due to its strong electronegativity, has a destructive effect on the surface. The rank of the adsorption ability of other three anions is Cl− > Br− > I− according to the value of adsorption energy, which is agreement with their electronegativity strength. It was found that the halogen anions exhibited excellent diffusion performance with low diffusion energy barriers. Cl− can adsorb up to three layer showing an excellent theoretical capacity of 415 mA h g−1, while Br− and I− cannot obtain a stable structure when the coverage exceeds 1 and (2/3) layer. In summary, this study evaluates a prospective electrode material and establishes a theoretical foundation for the development of novel rechargeable batteries.
{"title":"Theoretical Study of Halogen Anion Batteries With Ultra-Thin InSe","authors":"Xin Wei, Fengjun Liu, Mengyu Zhu, Lin Wang, Maolin Sha","doi":"10.1002/qua.70012","DOIUrl":"https://doi.org/10.1002/qua.70012","url":null,"abstract":"<div>\u0000 \u0000 <p>We systematically explored the adsorption, diffusion, thermodynamics stability, and electrochemical performance of halogen anions (F<sup>−</sup>, Cl<sup>−</sup>, Br<sup>−</sup>, I<sup>−</sup>) on monolayer InSe using first-principles calculations. F<sup>−</sup>, due to its strong electronegativity, has a destructive effect on the surface. The rank of the adsorption ability of other three anions is Cl<sup>−</sup> > Br<sup>−</sup> > I<sup>−</sup> according to the value of adsorption energy, which is agreement with their electronegativity strength. It was found that the halogen anions exhibited excellent diffusion performance with low diffusion energy barriers. Cl<sup>−</sup> can adsorb up to three layer showing an excellent theoretical capacity of 415 mA h g<sup>−1</sup>, while Br<sup>−</sup> and I<sup>−</sup> cannot obtain a stable structure when the coverage exceeds 1 and (2/3) layer. In summary, this study evaluates a prospective electrode material and establishes a theoretical foundation for the development of novel rechargeable batteries.</p>\u0000 </div>","PeriodicalId":182,"journal":{"name":"International Journal of Quantum Chemistry","volume":"125 3","pages":""},"PeriodicalIF":2.3,"publicationDate":"2025-01-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143117973","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}
Ali Almahmoud, Amer Almahmoud, Abdalla Obeidat, Maen Gharaibeh
Monte Carlo (MC) simulation and density functional theory (DFT) were employed to investigate the structural, mechanical, thermomagnetic, and electronic properties of the Co2CrGa1−xAlx (x = 0, 0.25, 0.50, 0.75, and 1.0) full Heusler alloys. Both the pristine and doped configurations demonstrate the L21 prototype, and there is an observable decrease in the lattice parameter as the Al concentration rises. Electronic analysis was performed in Wien2k using the Perdew–Burke–Ernzerhof of generalized gradient approximation (GGA-PBE), the modified Becke–Johnson GGA (mBJ-GGA), and the PBEsol functional, which revealed a band gap in the spin-down states of both structures by studying the band structure and density of states. The phonon dispersion relation was studied to ensure the stability of the alloy. The magnetic moments in pristine configurations closely resemble those in doped structures, with minimal changes in exchange interaction parameters. The obtained Curie temperature, determined through the MC method, falls within the range of 321–500 K. Finally, studying the magnetic properties of the Heusler alloys can contribute to advancements in spintronics and other magnetic applications.
{"title":"Studying the Structural, Electronic, and Magnetic Properties of Co2CrGa1 − xAlx Full Heusler Alloys Through Density Functional Theory and Monte Carlo Simulation","authors":"Ali Almahmoud, Amer Almahmoud, Abdalla Obeidat, Maen Gharaibeh","doi":"10.1002/qua.70013","DOIUrl":"https://doi.org/10.1002/qua.70013","url":null,"abstract":"<div>\u0000 \u0000 <p>Monte Carlo (MC) simulation and density functional theory (DFT) were employed to investigate the structural, mechanical, thermomagnetic, and electronic properties of the Co<sub>2</sub>CrGa<sub>1−<i>x</i></sub>Al<sub><i>x</i></sub> (<i>x</i> = 0, 0.25, 0.50, 0.75, and 1.0) full Heusler alloys. Both the pristine and doped configurations demonstrate the L2<sub>1</sub> prototype, and there is an observable decrease in the lattice parameter as the Al concentration rises. Electronic analysis was performed in Wien2k using the Perdew–Burke–Ernzerhof of generalized gradient approximation (GGA-PBE), the modified Becke–Johnson GGA (mBJ-GGA), and the PBEsol functional, which revealed a band gap in the spin-down states of both structures by studying the band structure and density of states. The phonon dispersion relation was studied to ensure the stability of the alloy. The magnetic moments in pristine configurations closely resemble those in doped structures, with minimal changes in exchange interaction parameters. The obtained Curie temperature, determined through the MC method, falls within the range of 321–500 K. Finally, studying the magnetic properties of the Heusler alloys can contribute to advancements in spintronics and other magnetic applications.</p>\u0000 </div>","PeriodicalId":182,"journal":{"name":"International Journal of Quantum Chemistry","volume":"125 3","pages":""},"PeriodicalIF":2.3,"publicationDate":"2025-01-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143118035","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}