scholarly journals The Near-ultraviolet Absorption Spectrum of Diimide Vapor

1974 ◽  
Vol 52 (6) ◽  
pp. 1006-1012 ◽  
Author(s):  
R. A. Back ◽  
C. Willis ◽  
D. A. Ramsay

Absorption spectra of N2H2 and N2D2 in the gas phase have been obtained in the region 3000–4300 Å, consisting of about 30 diffuse bands for each compound. Long progressions in the spectra are attributed to excitation of the H—N=N bending mode, v2′, in the upper state, with much shorter progressions arising from the N=N stretching mode, v3′; values of v2′ = 1215 and 910 cm−1 and v3′ = 1550 and 1440 cm−1 were estimated for N2H2 and N2D2 respectively.The spectra are attributed to the 1Bg ← 1Ag(π* ← n+) transition of trans diimide, probably made allowed by vibronic interaction. From Franck–Condon calculations the H—N=N angle in the upper state was estimated to be 132 ± 2°, an increase of 25° from the ground-state value; the increase in the N=N bond length was estimated to be about 0.05 Å.


1974 ◽  
Vol 52 (13) ◽  
pp. 2513-2515 ◽  
Author(s):  
R. A. Back ◽  
C. Willis

The near-ultraviolet absorption spectrum of diimide in liquid ammonia at −50 °C is shifted about 500 Å to the red compared with the gas-phase spectrum, with λmax = 4000 Å. The spectrum is also broadened and the vibrational structure largely obscured. It is suggested that hydrogen bonding is responsible for these changes.Diimide is much more stable in liquid ammonia between −65 and −38 °C than in the gas phase at room temperature. A first-order decay is observed with Arrhenius parameters of A = 1.9 × 103 s−1 and E = 6.6 kcal/mol; this is always preceded by a more rapid, higher-order initial decay which may be related to the rapid decomposition observed during vaporization.



1978 ◽  
Vol 56 (11) ◽  
pp. 1575-1578 ◽  
Author(s):  
R. A. Back ◽  
C. Willis ◽  
D. A. Ramsay

The absorption spectra of N2H2 and N2D2 in the region 3000–4300 Å have been re-examined with somewhat higher resolution than was used in earlier work. The vibrational assignments of the principal progressions are unchanged except for the revision of the vibrational numbering suggested by the calculations of Perić, Buenker, and Peyerimhoff in 1977. The transition is electronically forbidden (1Bg–1Ag) but is made vibronically allowed by excitation of one quantum of the antisymmetric stretching vibration ν4′(bu). Weaker progressions are induced by the torsional vibration ν4′(au) and the antisymmetric H—N—N bending vibration ν6′(bu). Agreement between experiment and theory is generally satisfactory though some significant discrepancies in Franck–Condon factors have been noted.





1972 ◽  
Vol 43 (3) ◽  
pp. 467-471 ◽  
Author(s):  
W.David Sheasley ◽  
C.Weldon Mathews




1968 ◽  
Vol 22 (6) ◽  
pp. 785-786 ◽  
Author(s):  
David N. Bailey ◽  
David K. Roe ◽  
David M. Hercules






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