Graduate School of Science, Hiroshima University, 1-3-1 Kagamiyama, Higashi-Hiroshima 739-8526, Japan.
J Chem Phys. 2012 Jan 7;136(1):014308. doi: 10.1063/1.3673778.
Nitrogen 1s (N 1s) core-to-Rydberg excitation spectra of hydrogen-bonded clusters of ammonia (AM) have been studied in the small cluster regime of beam conditions with time-of-flight (TOF) fragment-mass spectroscopy. By monitoring partial-ion-yield spectra of cluster-origin products, "cluster" specific excitation spectra could be recorded. Comparison of the "cluster" band with "monomer" band revealed that the first resonance bands of clusters corresponding to N 1s → 3sa(1)/3pe of AM monomer are considerably broadened. The changes of the experimental core-to-Rydberg transitions ΔFWHM (N 1s → 3sa(1)/3pe) = 0.20/0.50 eV compare well with the x ray absorption spectra of the clusters generated by using density functional theory (DFT) calculation. The broadening of the core-to-Rydberg bands in small clusters is interpreted as being primarily due to the splitting of non-equivalent core-hole N 1s states caused by both electrostatic core-hole and hydrogen-bonding (H(3)N···H-NH(2)) interactions upon dimerization. Under Cs dimer configuration, core-electron binding energy of H-N (H-donor) is significantly decreased by the intermolecular core-hole interaction and causes notable redshifts of core-excitation energies, whereas that of lone-pair nitrogen (H-acceptor) is slightly increased and results in appreciable blueshifts in the core-excitation bands. The result of the hydrogen-bonding interaction strongly appears in the n-σ* orbital correlation, destabilizing H-N donor Rydberg states in the direction opposite to the core-hole interaction, when excited N atom with H-N donor configuration strongly possesses the Rydberg component of anti-bonding σ* (N-H) character. Contributions of other cyclic H-bonded clusters (AM)(n) with n ≥ 3 to the spectral changes of the N 1s → 3sa(1)/3pe bands are also examined.
已在飞行时间(TOF)碎片质谱的束条件的小团簇范围内研究了氨(AM)氢键团簇的氮 1s(N 1s)核心到里德堡激发光谱。通过监测团簇源产物的部分离子产率光谱,可以记录“团簇”特定的激发光谱。将“团簇”带与“单体”带进行比较,发现对应于 AM 单体的 N 1s→3sa(1)/3pe 的第一共振带的团簇的第一共振带明显展宽。实验的核心到里德堡跃迁的变化 ΔFWHM(N 1s→3sa(1)/3pe)=~0.20/0.50 eV 与使用密度泛函理论(DFT)计算生成的团簇的 X 射线吸收光谱非常吻合。小团簇中核心到里德堡带的展宽主要解释为静电核孔和氢键(H(3)N···H-NH(2))相互作用引起的非等效核孔 N 1s 态的分裂。在 Cs 二聚体构型下,分子间核孔相互作用使 H-N(H-供体)的核心电子结合能显著降低,并导致核心激发能显著红移,而孤对氮(H-受体)的核心电子结合能略有增加,并导致核心激发带明显蓝移。氢键相互作用的结果强烈出现在 n-σ轨道相关中,当具有 H-N 供体构型的激发 N 原子强烈具有反键σ(N-H)性质的里德堡分量时,以与核孔相互作用相反的方向使 H-N 供体里德堡态失稳。还研究了其他具有 n≥3 的环状氢键团簇(AM)(n)对 N 1s→3sa(1)/3pe 带光谱变化的贡献。