Calculated Magnetic and Geometric Structures of Neutral Copper Oxide Clusters

IF 2.8 2区 化学 Q3 CHEMISTRY, PHYSICAL
Chase H. Rotteger, , , Hannah G. Rucker, , , Madison M. Sobol, , and , Scott G. Sayres*, 
{"title":"Calculated Magnetic and Geometric Structures of Neutral Copper Oxide Clusters","authors":"Chase H. Rotteger,&nbsp;, ,&nbsp;Hannah G. Rucker,&nbsp;, ,&nbsp;Madison M. Sobol,&nbsp;, and ,&nbsp;Scott G. Sayres*,&nbsp;","doi":"10.1021/acs.jpca.5c04015","DOIUrl":null,"url":null,"abstract":"<p >The ground state geometric structures and electron configurations of subnanometer neutral copper oxide clusters are calculated with density functional theory. By comparing the results across almost 40 clusters, ranging between Cu<sub>3</sub>O<sub>3</sub> and Cu<sub>16</sub>O<sub>8</sub>, we find evidence for strong ferromagnetic coupling that is responsible for increasing the number of unpaired electrons as Cu atoms are incremented away from the (Cu<sub>2</sub>O)<i><sub>n</sub></i> stoichiometry. The closed-shell (Cu<sub>2</sub>O)<i><sub>n</sub></i> clusters are nonmagnetic, whereas all other clusters exhibit varying degrees of magnetic susceptibility. The majority of the clusters considered in this manuscript have not been previously evaluated. Natural bonding orbital and Bader charge analysis reveal a nearly linear correlation between the charge transfer between Cu and O atoms and their local spin magnetic moments. Further, a relationship between the coordination of O atoms composing the cluster and their local magnetic moment is found. Bridging O atoms (μ2-O) typically exhibit large local magnetic moments, whereas the local magnetic moment is quenched by tetrahedrally coordinated (μ4-O) atoms. Thus, clusters containing Cu(II) atoms contain a large total magnetic moment, whereas Cu(I) atom clusters generally exhibit a small total magnetic moment and terminal Cu atom structures.</p>","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":"129 39","pages":"8982–8992"},"PeriodicalIF":2.8000,"publicationDate":"2025-09-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Journal of Physical Chemistry A","FirstCategoryId":"1","ListUrlMain":"https://pubs.acs.org/doi/10.1021/acs.jpca.5c04015","RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0

Abstract

The ground state geometric structures and electron configurations of subnanometer neutral copper oxide clusters are calculated with density functional theory. By comparing the results across almost 40 clusters, ranging between Cu3O3 and Cu16O8, we find evidence for strong ferromagnetic coupling that is responsible for increasing the number of unpaired electrons as Cu atoms are incremented away from the (Cu2O)n stoichiometry. The closed-shell (Cu2O)n clusters are nonmagnetic, whereas all other clusters exhibit varying degrees of magnetic susceptibility. The majority of the clusters considered in this manuscript have not been previously evaluated. Natural bonding orbital and Bader charge analysis reveal a nearly linear correlation between the charge transfer between Cu and O atoms and their local spin magnetic moments. Further, a relationship between the coordination of O atoms composing the cluster and their local magnetic moment is found. Bridging O atoms (μ2-O) typically exhibit large local magnetic moments, whereas the local magnetic moment is quenched by tetrahedrally coordinated (μ4-O) atoms. Thus, clusters containing Cu(II) atoms contain a large total magnetic moment, whereas Cu(I) atom clusters generally exhibit a small total magnetic moment and terminal Cu atom structures.

Abstract Image

计算中性氧化铜团簇的磁性和几何结构。
用密度泛函理论计算了亚纳米中性氧化铜团簇的基态几何结构和电子构型。通过比较Cu3O3和Cu16O8之间近40个簇的结果,我们发现了强铁磁耦合的证据,当Cu原子逐渐远离(Cu2O)n化学计量时,强铁磁耦合导致了未配对电子数量的增加。闭壳(Cu2O)n团簇是非磁性的,而所有其他团簇都表现出不同程度的磁化率。在这篇手稿中考虑的大多数集群以前没有被评估过。自然成键轨道和Bader电荷分析揭示了Cu和O原子之间的电荷转移与其局部自旋磁矩之间的线性关系。此外,还发现了组成团簇的O原子的配位与它们的局部磁矩之间的关系。桥接O原子(μ2-O)具有较大的局域磁矩,而局域磁矩被四面体配位原子(μ4-O)猝灭。因此,含有Cu(II)原子的团簇具有较大的总磁矩,而Cu(I)原子团簇通常具有较小的总磁矩和末端Cu原子结构。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
The Journal of Physical Chemistry A
The Journal of Physical Chemistry A 化学-物理:原子、分子和化学物理
CiteScore
5.20
自引率
10.30%
发文量
922
审稿时长
1.3 months
期刊介绍: The Journal of Physical Chemistry A is devoted to reporting new and original experimental and theoretical basic research of interest to physical chemists, biophysical chemists, and chemical physicists.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信