Microwave spectrum, dipole moment and AB initio structure of iminopyruvonitrile (CH3C(CN)NH)

1987 ◽  
Vol 139 (5) ◽  
pp. 479-484 ◽  
Author(s):  
P. Groner ◽  
R. Gunde ◽  
T.-K. Ha ◽  
A. Bauder
Keyword(s):  
Dipole Moment ◽  
Ab Initio ◽  
Microwave Spectrum ◽  
Ab Initio Structure

scholarly journals Microwave Spectrum, Dipole Moment, Planarity and Stability of syn-Oxalyl Fluoride. Ab Initio Computations of the anti--syn Equilibrium of Oxalyl Fluoride.

1995 ◽  
Vol 49 ◽  
pp. 172-181 ◽  
Author(s):  
K.-M. Marstokk ◽  
Harald Møllendal ◽  
Sture Nordholm ◽  
Per Halfdan Nielsen ◽  
Alf Claesson ◽  
...  
Keyword(s):  
Dipole Moment ◽  
Ab Initio ◽  
Microwave Spectrum ◽  
Ab Initio Computations

Bond order-bond length relationships in conjugated hydrocarbons - the microwave spectrum and structure of 3,4-dimethylenecyclobutene

1983 ◽  
Vol 36 (4) ◽  
pp. 639 ◽  
Author(s):  
RD Brown ◽  
PD Godfry ◽  
BT Hart ◽  
AL Ottrey ◽  
M Onda ◽  
...  
Keyword(s):  
Dipole Moment ◽  
Ab Initio ◽  
Bond Length ◽  
Bond Order ◽  
Microwave Spectrum ◽  
Basis Set ◽  
Molecular Orbital Calculations ◽  
Bond Orders ◽  
Bond Lengths ◽  
Typical Error

The microwave spectrum of the benzene isomer 3,4-dimethylenecyclobutene including spectra of all possible single 13C-substituted and sufficient singly and doubly D-substituted species to give a complete r5 geometry, have been measured and analysed. An estimate of the re geometry has also been derived. The additional precise CC bond lengths obtained for an unsubstituted, conjugated hydrocarbon enable us to examine bond order-bond length relationships more thoroughly than has previously been possible. The CC bond lengths exhibit a noticeably better correlation with SCFMO bond orders than with simple H�ckel bond orders. Further confirmatory measurements of the dipole moment of dimethylenecyclobutene have been made. Ab initio molecular orbital calculations using a 6-31G basis set give an optimized geometry with CC bond lengths within 2 pm of the r5 values. The computed dipole moment agrees almost exactly with experiment but a corresponding calculation on fulvene is discrepant with experiment by 0.16 D, which is probably a more typical error.

Microwave Spectrum,r0Structure, Dipole Moment, Barrier to Internal Rotation, and Ab Initio Calculations for Fluoromethylsilane

2010 ◽  
Vol 114 (12) ◽  
pp. 4131-4137 ◽  
Author(s):  
James R. Durig ◽  
Savitha S. Panikar ◽  
Peter Groner ◽  
Hossein Nanaie ◽  
Hans Bürger ◽  
...  
Keyword(s):  
Dipole Moment ◽  
Ab Initio Calculations ◽  
Ab Initio ◽  
Internal Rotation ◽  
Microwave Spectrum

Ab initio structure determination of cytochrome c6 by combined reciprocal space-real space approach

2003 ◽  
Vol 218 (1) ◽  
Author(s):  
K. Chowdhury ◽  
S. Ghosh ◽  
M. Mukherjee
Keyword(s):  
Cytochrome C ◽  
Ab Initio ◽  
Structure Determination ◽  
Direct Method ◽  
Real Space ◽  
Reciprocal Space ◽  
Cytochrome C6 ◽  
Ab Initio Structure ◽  
Space Approach

AbstractThe direct method program SAYTAN has been applied successfully to redetermine the structure of cytochrome c

Microwave spectrum, dipole moment, and conformation of ethanedithiol

1984 ◽  
Vol 81 (2) ◽  
pp. 1051-1053 ◽  
Author(s):  
R. N. Nandi ◽  
Chun‐Fu Su ◽  
Marlin D. Harmony
Keyword(s):  
Dipole Moment ◽  
Microwave Spectrum

scholarly journals The Microwave Spectrum of 3,4-Dihydro-1,2-Pyran

1985 ◽  
Vol 40 (9) ◽  
pp. 913-919
Author(s):  
Juan Carlos López ◽  
José L. Alonso
Keyword(s):  
Dipole Moment ◽  
Excited States ◽  
Ground State ◽  
Principal Axis ◽  
Microwave Spectrum ◽  
Average Intensity ◽  
Ring Conformation ◽  
Vibrationally Excited ◽  
Rotational Constants ◽  
Displacement Measurements

Abstract The rotational transitions of 3,4-dihydro-1,2-pyran in the ground state and six vibrationally excited states have been assigned. The rotational constants for the ground state (A = 5198.1847(24), B = 4747.8716(24) and C = 2710.9161(24) have been derived by fitting μa, μb and μc-type transitions. The dipole moment was determined from Stark displacement measurements to be 1.400(8) D with its principal axis components |μa| =1.240(2), |μb| = 0.588(10) and |μc| = 0.278(8) D. A model calculation to reproduce the ground state rotational constants indicates that the data are consistent with a twisted ring conformation. The average intensity ratio gives vibrational separations between the ground and excited states of the ring-bending and ring-twisting modes of ~ 178 and ~ 277 cm-1 respectively.

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