The excited states of azulene: A study of the vibrational energy levels for the lower ππ*-valence states by configuration interaction and density functional calculations, and theoretical studies of the Rydberg states

被引:3
|
作者
Palmer, Michael H. [1 ]
Jones, Nykola C. [2 ]
Hoffmann, Soren Vronning [2 ]
Aitken, R. Alan [3 ]
Coreno, Marcello [4 ]
de Simone, Monica [5 ]
Grazioli, Cesare [5 ]
Patterson, Iain L. J. [3 ]
机构
[1] Univ Edinburgh, Sch Chem, Joseph Black Bldg,David Brewster Rd, Edinburgh EH9 3FJ, Scotland
[2] Aarhus Univ, Dept Phys & Astron, ISA, Ny Munkegade 120, DK-8000 Aarhus C, Denmark
[3] Univ St Andrews, Sch Chem, St Andrews Fife KY16 9ST, Scotland
[4] Inst Struttura Mat ISM CNR, LD2 Unit, I-34149 Trieste, Italy
[5] Ist Officina Materiali, IOM CNR, Basovizza SS-14,Km 163-5, I-34149 Trieste, Italy
来源
JOURNAL OF CHEMICAL PHYSICS | 2022年 / 157卷 / 15期
关键词
JET-COOLED AZULENE; CLUSTER-EXPANSION; ABSORPTION-SPECTRUM; WAVE-FUNCTION; ELECTRON CORRELATIONS; INTERNAL-CONVERSION; HERZBERG-TELLER; NAPHTHALENE; IONIZATION; SYMMETRY;
D O I
10.1063/5.0106697
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
A new vacuum ultraviolet absorption (VUV) spectrum of azulene vapor has been obtained by using a synchrotron radiation source. The onset of the ultraviolet spectrum, previously reported by Sidman et al., has been analyzed in detail by Franck-Condon (FC) and Herzberg-Teller (HT) methods. The photoelectron spectral profile identifies the 3px-Rydberg state 0(0) band to be 131 cm(-1) from the VUV maximum. Excited state energy levels were calculated by three independent methods: the wide scan VUV spectrum was correlated with symmetry adapted cluster configuration interaction calculations. The low energy portion of the spectrum was studied by both time dependent density functional theoretical methods (TDDFT) and multi-reference multi-root CI (MRD-CI). Equilibrium structures were determined for valence states at the TDDFT level. Rydberg states were determined by both TDDFT and MRD-CI. The FC + HT analyses were performed on the TDDFT wave-functions. The HT intensity profiles are generally low in intensity, relative to the FC ones; however, HT is dominant in the second singlet state (S-2, 1(1)A(1)). As a result, numerous non-symmetric modes, their overtones, and combination bands show considerable intensity in that band. Energies obtained from use of extremely diffuse s-, p-, d-, or f-character functions enabled realistic extrapolation to the IE1 for many Rydberg states (RS). The lowest RS (3b(1)3s) based on IE2 lies at 4.804 eV with a quantum defect of 0.714. Differentiation between valence and RS is readily made using the second moments of the charge distribution. Published under an exclusive license by AIP Publishing.
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页数:15
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