搜索

x
中国物理学会期刊

\bf Ta_4C_\boldsymbol n^\bf -/0 (n = 0—4)团簇的电子结构、成键性质及稳定性

CSTR: 32037.14.aps.70.20201351

Electronic structures, chemical bonds, and stabilities of \rmTa_4\rmC_n^-/0 (n = 0–4) clusters: Anion photoelectron spectroscopy and theoretical calculations

CSTR: 32037.14.aps.70.20201351
PDF
HTML
导出引用
  • 本文采用尺寸选择的负离子光电子能谱技术, 结合密度泛函理论, 对\rmTa_4\rmC_n^-/0 (n = 0—4)团簇电子结构、成键性质以及稳定性进行了研究. 实验测得\rmTa_4\rmC_n^- (n = 0—4)团簇负离子基态结构的垂直脱附能分别为(1.16 ± 0.08), (1.35 ± 0.08), (1.51 ± 0.08), (1.30 ± 0.08)和(1.86 ± 0.08) eV. 中性Ta4Cn (n = 0—4)团簇的电子亲和能分别为(1.10 ± 0.08), (1.31 ± 0.08), (1.44 ± 0.08), (1.21 ± 0.08)和(1.80 ± 0.08) eV. 研究发现, \rmTa_4^-/0 团簇为四面体结构, \rmTa_4\rmC_1^-/0 团簇中碳原子覆盖在Ta4四面体的一个面上方, \rmTa_4\rmC_2^-/0 团簇则是两个碳原子分别覆盖在Ta4四面体中的两个面上方. \rmTa_4\rmC_3^-/0 团簇是一个缺角立方体结构. \rmTa_4\rmC_4^-/0 团簇则是近似立方体结构, 可以看成是α-TaC面心立方晶体的最小晶胞单元. 分子轨道分析结果显示\rmTa_4\rmC_3^- 团簇的单电子最高占据轨道主要布居在单个钽原子周围, 导致\rmTa_4\rmC_3^- 团簇的垂直脱附能明显低于其相邻团簇. 理论研究显示随着碳原子数目的增加, \rmTa_4\rmC_n^-/0 (n = 0—4)团簇中的钽-钽金属键逐渐被钽-碳共价键取代, 单原子结合能逐渐增加且明显高于\rmTa_4+n^-/0 (n = 0—4)团簇. 中性Ta4C4的单原子结合能高达7.13 eV, 这说明钽-碳共价键的形成有利于提高材料的熔点, 这与碳化钽作为高温陶瓷材料的特性密切相关.

     

    The electronic structures, chemical bonds and stabilities of \rmTa_4\rmC_n^-/0 (n = 0–4) clusters are investigated by combining anion photoelectron spectroscopy with theoretical calculations. The vertical detachment energy values of \rmTa_4\rmC_n^- (n = 0–4) anions are measured to be (1.16 ± 0.08), (1.35 ± 0.08), (1.51 ± 0.08), (1.30 ± 0.08), and (1.86 ± 0.08) eV, and the electron affinities of neutral Ta4Cn (n = 0–4) are estimated to be (1.10 ± 0.08), (1.31 ± 0.08), (1.44 ± 0.08), (1.21 ± 0.08), and (1.80 ± 0.08) eV, respectively. It is found that the geometry structure of \rmTa_4^- cluster is a tetrahedron, and the most stable structure of \rmTa_4\rmC_1^- has a carbon atom capping one face of the \rmTa_4^- tetrahedron, while in the ground state structure of \rmTa_4\rmC_2^- cluster, two carbon atoms cap two faces of the\rmTa_4^- tetrahedron, respectively. The lowest-lying isomer of \rmTa_4\rmC_3^- cluster holds a cube-cutting-angle structure. The ground state structure of \rmTa_4\rmC_4^- is a 2 × 2 × 2 cube. The neutral Ta4Cn (n = 0–4) clusters have similar structures to their anionic counterparts and the neutral Ta4C4 cluster can be considered as the smallest cell for α-TaC face-centered cube crystal. The analyses of molecular orbitals reveal that the SOMO of \rmTa_4\rmC_3^- is mainly localized on one tantalum atom, inducing a low VDE. Our results show that the Ta-Ta metal bonds are replaced by Ta-C covalent bonds gradually as the number of carbon atoms increases in \rmTa_4\rmC_n^-/0 (n = 0–4) clusters. The per-atom binding energy values of \rmTa_4\rmC_n^-/0 (n = 0–4) clusters are higher than those of \rmTa_4+n^-/0 (n = 0–4) clusters, indicating that the formation of Ta-C covalent bonds may raise the melting point. The per-atom binding energy of neutral Ta4C4 is about 7.13 eV, which is quite high, which may contribute to the high melting point of α-TaC as an ultra-high temperature ceramic material.

     

    目录

    /

    返回文章
    返回