Gas-Phase Molecular Geometry

2019 ◽  
pp. 111-123
Author(s):  
Gianluca Levi
Keyword(s):  
Gas Phase ◽  
Molecular Geometry

Molecular Geometry of Vanadium Dichloride and Vanadium Trichloride: A Gas-Phase Electron Diffraction and Computational Study

2010 ◽  
Vol 49 (6) ◽  
pp. 2816-2821 ◽  
Author(s):  
Zoltán Varga ◽  
Brian Vest ◽  
Peter Schwerdtfeger ◽  
Magdolna Hargittai
Keyword(s):  
Electron Diffraction ◽  
Gas Phase ◽  
Computational Study ◽  
Molecular Geometry ◽  
Gas Phase Electron Diffraction

Gas-phase vibrational spectrum and molecular geometry of TeCl4

1997 ◽  
pp. 1037-1042 ◽  
Author(s):  
Attila Kovács ◽  
Kjell-Gunnar Martinsen ◽  
Rudy J. M. Konings
Keyword(s):  
Vibrational Spectrum ◽  
Gas Phase ◽  
Molecular Geometry

Solid-State Modeling. VI. 2,3-Diketopiperazine: the Integration of Crystallographic and Spectroscopic Evidence

1998 ◽  
Vol 54 (6) ◽  
pp. 859-865 ◽  
Author(s):  
A. T. H. Lenstra ◽  
B. Bracke ◽  
B. van Dijk ◽  
S. Maes ◽  
C. Van Alsenoy ◽  
...  
Keyword(s):  
Solid State ◽  
Ab Initio ◽  
Gas Phase ◽  
Molecular Geometry ◽  
Membered Ring ◽  
Monoclinic Space Group ◽  
Boat Conformation ◽  
State Structure ◽  
Normal Vibrations ◽  
Spectral Changes

2,3-Diketopiperazine (2,3-piperazinedione) crystallizes in the monoclinic space group P21/c with a = 5.941 (3), b = 10.080 (3), c = 8.282 (2) Å and β = 95.87 (3)°. The six-membered ring adopts a skew-boat conformation with Q = 0.467 (3) Å, θ = 64.6 (3)° and φ = 269.8 (4)°. Ab initio calculations show that the perfect skew-boat with its C 2 symmetry is broken by the formation of two intermolecular N—H...O bonds, involving only one of the C=O groups of the 2,3-diketopiperazine molecule. Vibrational spectra were recorded in solution and in the solid state. The assignment of the normal vibrations is proposed based on comparison with spectra of similar molecules and spectral changes due to deuteration. Ab initio calculations for the isolated molecule and the solid-state structure were used to calculate differences in the molecular geometry in the gas phase and crystalline state. Using these reference structures we calculated the stretching frequencies for the C=O groups. We predict an IR shift for C=O of 130 cm−1, when the molecule goes from the gas phase to the solid state. The observed shift is 110 cm−1. The differences between the C=O moieties in the solid state produce a calculated Δν of 55 cm−1, which matches satisfactorily the observed value of 49 cm−1.

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