Bicyclo[3.2.0]hepta-1,3,6-triene — UV photoelectron spectroscopic and computational studies

2005 ◽  
Vol 83 (9) ◽  
pp. 1352-1359 ◽  
Author(s):  
T Bajorek ◽  
N H Werstiuk

Pyrolysis of N,N-dimethylbicyclo[3.2.0]hepta-3,6-dien-1-amine oxide (5) at 120 °C in the source chamber of the UV photoelectron (PE) spectrometer yielded bicyclo[3.2.0]hepta-1,3,6-triene (6). The triene dimerizes to yield a mixture of two dimers in equal amounts. A PE spectrum of an authentic mixture of dimers was also recorded for the purpose of spectral subtraction. Pyrolysis of 5 also generates dimethylhydroxylamine (7), a spectrum of which was also recorded from an authentic sample. Spectral subtraction allowed the first two ionization potentials of triene 6 at 7.2 and 9.8 eV to be identified. The resultant PE spectrum was compared very favorably with a simulated spectrum obtained from DFT calculations. A QTAIM analysis and calculation of delocalization indexes showed that while homoconjugation between C4 and C6 is negligible there is a weak through-space interaction between the bridgehead carbon atom C1 and C6 of the four-membered ring.Key words: bicyclo[3.2.0]hepta-1,3,6-triene, UV photoelectron spectroscopy, DFT calculations, QTAIM, delocalization indexes.

2004 ◽  
Vol 82 (2) ◽  
pp. 80-86 ◽  
Author(s):  
Tom Bajorek ◽  
Nick H Werstiuk

The photoelectron spectra of N,N-dimethylbicyclo[3.2.0]hepta-3,6-dien-1-amine (1) and its pyrolysate were obtained using an unique ultraviolet (UV) photoelectron (PE) spectrometer interfaced with a CW CO2 laser. Pyrolysis of 1 in the source chamber of the PE spectrometer initially generates the transient N,N-dimethylcyclohepta-1E,3Z,5Z-trien-1-amine (2) — the computed barrier is 21.5 kcal mol–1 — that isomerizes to the all-cis isomer with a barrier of only 5.0 kcal mol–1. There is no evidence for the formation of N,N-dimethycyclohepta-1Z,3E,5Z-trien-1-amine (4), formation of which has an zero-point-energy corrected barrier of 28.4 kcal mol-1. A PE spectrum of an authentic sample of N,N-dimethylcyclohepta-1Z,3Z,5Z-trien-1-amine (3) correlated well with the pyrolysis spectrum. Molecular orbitals and their energies were obtained with Becke3LYP calculations.Key words: vacuum pyrolysis, N,N-dimethylbicyclo[3.2.0]hepta-3,6-dien-1-amine, photoelectron spectroscopy, DFT calculations.


1985 ◽  
Vol 50 (3) ◽  
pp. 650-657 ◽  
Author(s):  
Tomáš Juška

The UV photoelectron spectra of isomeric para and meta derivatives of benzonitrile with substituents NO2, COCH3, Cl, Br, CH2I and NH2 were measured. Their assignment was carried out with the aid of MNDO calculations. The splitting of the highest π orbitals e1gS, e1gA is in all para derivatives greater than in their meta isomers, the greatest difference of splittings 0.25 eV being caused by the amino group. The level ordering e1gS, A exists in all molecules except meta NO2, and COCH3 derivatives where it is believed to be reverse. The π'CN - πCN splitting keeps nearly constant and it is close to that in benzonitrile. The ionization potentials of σ orbitals e1uS, e1uA, b2u and b1u in meta NO2 derivative are, in agreement with our expectation, higher than in benzonitrile. It is not true for para isomer where on the contrary, they are lower and they differ from meta isomer by 0.71-1.8 eV.


2001 ◽  
Vol 595 (1-3) ◽  
pp. 139-146 ◽  
Author(s):  
Karinne Miqueu ◽  
Jean-Marc Sotiropoulos ◽  
Geneviève Pfister-Guillouzo ◽  
Henri Ranaivonjatovo ◽  
Jean Escudié

2008 ◽  
Vol 91 (4) ◽  
pp. 766-781 ◽  
Author(s):  
Tomasz Drewnowski ◽  
Anna Chrostowska ◽  
Stanisław Leśniak ◽  
Alain Dargelos ◽  
Saïd Khayar

ChemInform ◽  
2010 ◽  
Vol 22 (45) ◽  
pp. no-no
Author(s):  
G. DISTEFANO ◽  
M. DAL COLLE ◽  
V. BERTOLASI ◽  
P. R. OLIVATO ◽  
E. BONFADA ◽  
...  

Tetrahedron ◽  
2009 ◽  
Vol 65 (51) ◽  
pp. 10581-10589 ◽  
Author(s):  
Stanisław Leśniak ◽  
Anna Chrostowska ◽  
Dawid Kuc ◽  
Małgorzata Maciejczyk ◽  
Saïd Khayar ◽  
...  

Data on calculated orbital energies and experimentally measured ionization potentials of carbocyclic and heterocyclic aromatic compounds are compared and contrasted. The ordering or orbital energies and ionization potentials do not always seem to parallel one another, probably owing to either electron correlation effects, or to deviations from Koopman’s theorem. The effects on photoelectron spectra of using different light sources and analysers are discussed in relation to their bearing on the orbital orderings of aromatic compounds. The high resolution He 584 A. photoelectron spectrum of pyridine is shown to be open to two interpretations regarding the ordering of the ionization potentials of the π orbitals and the ‘nitrogen lone pair’ (n). One of the interpretations involves the three lowest pyridine ionization potentials being π (9.2 eV), π L (9.5 eV) and n (10.5 eV) whilst the other has the first three ionization potentials being the order π , n, π . The photoelectron spectra of substituted pyridines and diazines are discussed in the light of the two possible explanations for the pyridine spectrum.


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