High-resolution infrared studies of the ν10, ν11, ν14, and ν18 levels of [1.1.1]propellane

被引:3
|
作者
Kirkpatrick, Robynne [1 ]
Masiello, Tony [2 ]
Martin, Matthew [1 ]
Nibler, Joseph W. [1 ]
Maki, Arthur
Weber, Alfons [3 ]
Blake, Thomas A. [4 ]
机构
[1] Oregon State Univ, Dept Chem, Corvallis, OR 97332 USA
[2] Calif State Univ Hayward, Dept Chem & Biochem, Hayward, CA 94542 USA
[3] NIST, Sensor Sci Div, Gaithersburg, MD 20899 USA
[4] Pacific NW Natl Lab, Richland, WA 99352 USA
关键词
Propellane; High-resolution infrared spectrum; Rovibrational constants; Coriolis interactions; Ground state structure; DFT calculations; Anharmonic frequencies; SYMMETRIC-TOP MOLECULES; SPECTROSCOPY; PROPELLANES;
D O I
10.1016/j.jms.2012.09.001
中图分类号
O64 [物理化学(理论化学)、化学物理学]; O56 [分子物理学、原子物理学];
学科分类号
070203 ; 070304 ; 081704 ; 1406 ;
摘要
This paper is a continuation of earlier work in which the high resolution infrared spectrum of [1.1.1]propellane was measured and its k and l structure resolved for the first time. Here we present results from an analysis of more than 16000 transitions involving three fundamental bands nu(10) (E' - A'(1)), nu(11) (E' - A'(1)) nu(14) (A ''(2) A'(1)) and two difference bands (nu(10)-nu(18)) (E'-E '') and (nu(11) - nu(18)) (E' - E ''). Additional information about nu(18) was also obtained from the difference band (nu(15) + v18) - v18 (E' - E '') and the binary combination band (nu(15) + nu(18)) (E' - A'(1)). Through the use of the ground state constants reported in an earlier paper [11, rovibrational constants have been determined for all the vibrational states involved in these bands. The rovibrational parameters for the nu(18) (The rovibrational parameters for the nu(18) (E '') state were obtained from combination-differences and) state were obtained from combination-differences and showed no need to include interactions with other states. The nu(10) (E') state analysis was also straight-forward, with only a weak Coriolis interaction with the levels of the nu(14) (A) state. The latter levels are much more affected by a strong Coriolis interaction with the levels of the nearby nu(11) (E') state and also by a small but significant interaction with another state, presumably the nu(18) (E '') state, that is not directly observed. Gaussian calculations (B3LYP/cc-pVTZ) computed at the anharmonic level aided the analyses by providing initial values for many of the parameters. These theoretical results generally compare favorably with the final parameter values deduced from the spectral analyses. Finally, evidence was obtained for several level crossings between the rotational levels of the nu(11) and nu(14) states and, using a weak coupling term corresponding to a Delta k = 5, Delta/= -/+ 1 matrix element, it was possible to find transitions from the ground state that, combined with transitions to the same upper state, give a value of C-o = 0.1936515(4) cm(-1). This result, combined with the value of B-o = 0.28755833(14) cm(-1) reported earlier Ill, yields a value of 1.586277(3) A for the length of the novel axial CC bond in propellane. (C) 2012 Elsevier Inc. All rights reserved.
引用
收藏
页码:51 / 62
页数:12
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