Liao Hsin-Yi, Tsuge Masashi, Tan Jake A, Kuo Jer-Lai, Lee Yuan-Pern
Department of Science Education, National Taipei University of Education, 134, Section 2, Heping East Road, Daan District, Taipei 10659, Taiwan.
Phys Chem Chem Phys. 2017 Aug 9;19(31):20484-20492. doi: 10.1039/c7cp03847j.
The proton-bound nitrogen dimer, N-H-N, and its isotopologues were investigated by means of vibrational spectroscopy. These species were produced upon electron bombardment of mixtures of N (or N) and para-hydrogen (p-H) or normal-D (n-D) during deposition at 3.2 K. Reduced-dimension anharmonic vibrational Schrödinger equations were constructed to account for the strong anharmonic effects in these protonated species. The fundamental lines of proton motions in N-H-N were observed at 715.0 (NHN antisymmetric stretch, ν), 1129.6 (NHN bend, ν), and 2352.7 (antisymmetric NN/NN stretch, ν) cm, in agreement with values of 763, 1144, and 2423 cm predicted with anharmonic calculations using the discrete-variable representation (DVR) method at the CCSD/aug-cc-pVDZ level. The lines at 1030.2 and 1395.5 cm were assigned to combination bands involving nν + ν (n = 1 and 2) according to theoretical calculations; ν is the NN stretching mode. For N-H-N in solid p-H, the corresponding major lines were observed at 710.0 (ν), 1016.7 (ν + ν), 1124.3 (ν), 1384.8 (2ν + ν), and 2274.9 (ν) cm. For N-D-N in solid n-D, the corresponding major lines were observed at 494.0 (ν), 840.7 (ν + ν), 825.5 (ν), and 2356.2 (ν) cm. In addition, two lines at 762.0 (weak) and 808.3 cm were tentatively assigned to be some modes of N-H-N perturbed or activated by a third N near the proton.
通过振动光谱法对质子结合的氮二聚体N-H-N及其同位素进行了研究。这些物种是在3.2 K沉积过程中,对N(或N)与对氢(p-H)或正氘(n-D)的混合物进行电子轰击时产生的。构建了降维非谐振动薛定谔方程,以解释这些质子化物种中的强非谐效应。在715.0 cm(NHN反对称伸缩振动,ν)、1129.6 cm(NHN弯曲振动,ν)和2352.7 cm(反对称NN/NN伸缩振动,ν)处观测到了N-H-N中质子运动的基频线,这与使用离散变量表示(DVR)方法在CCSD/aug-cc-pVDZ水平进行非谐计算预测的763、1144和2423 cm的值一致。根据理论计算,1030.2和1395.5 cm处的谱线被归为涉及nν + ν(n = 1和2)的组合带;ν是NN伸缩模式。对于固体p-H中的N-H-N,在710.0 cm(ν)、1016.7 cm(ν + ν)、1124.3 cm(ν)、1384.8 cm(2ν + ν)和2274.9 cm(ν)处观测到了相应的主要谱线。对于固体n-D中的N-D-N,在494.0 cm(ν)、840.7 cm(ν + ν)、825.5 cm(ν)和2356.2 cm(ν)处观测到了相应的主要谱线。此外,762.0 cm(弱)和808.3 cm处的两条谱线被初步归为质子附近第三个N对N-H-N产生扰动或激活的某些模式。