The electronic absorption spectrum of NHD

1979 ◽  
Vol 57 (5) ◽  
pp. 761-766 ◽  
Author(s):  
D. A. Ramsay ◽  
F.D. Wayne

Rotational assignments are given for about 350 lines in the (0,9,0)–(0,0,0), (0,10,0)–(0,0,0), and (0,11,0)–(0,0,0) bands in the electronic absorption spectrum of NHD. The Σ and Δ sub-bands have been identified for the bands with ν2′ odd and the Π sub-band for the band with ν2′ even.Ground state rotational and spin–rotational constants have been determined. The principal constants in reciprocal centimetres are: A = 20.1162(32), B = 8.1114(16), C = 5.6681(16), εaa = −0.2324(51),εbb = −0.0373ε, εcc = −0.0019ε, where the error limits are 1σ. Term values are tabulated for both the ground and excited state levels.Several 'axis-switching' branches have been identified in agreement with the predictions of Hougen and Watson.


1968 ◽  
Vol 46 (23) ◽  
pp. 2619-2631 ◽  
Author(s):  
R. N. Dixon ◽  
D. A. Ramsay

Absorption bands of NCS between 3300 Å and 4000 Å have been assigned to two electronic band systems, A(2Πi) – X(2Πi) with its origin at 26 054 cm−1, and B(2Σ+) – X(2Πi) with its origin at 26 844 cm−1. Rotational analyses have been carried out for the stronger bands, yielding rotational constants B0 = 0.2036 cm−1 (A state), B0 = 0.1906 cm−1 (A state), and B0 = 0.1969 cm−1 (B state). In addition to vibronic interactions within the two 2Πi states (Renner effect) there is considerable evidence for vibronic interaction between the A(2Πi) and B(2Σ+) states.



2009 ◽  
Vol 74 (5) ◽  
pp. 1084-1089 ◽  
Author(s):  
Jin-Ling Song ◽  
Li-Ming Gong ◽  
Shou-Ai Feng ◽  
Jiang-Hong Zhao ◽  
Jian-Feng Zheng ◽  
...  


An electronic absorption spectrum, attributed to phenyl, has been observed in the visible region with origin at 18 908 cm -1 after flash photolysis of benzene and halogenobenzenes. Similar spectra of fluoro, chloro and bromo phenyl are observed after flash photolysis of disubstituted benzenes. The vibrational structure of the phenyl spectrum has been analysed in terms of two fundamental frequencies at 571 and 896 cm -1 which correspond to the e 2 g and a 1 g frequencies of the B 2 u state of benzene. The ground state of phenyl has a π 6 n electronic configuration and the observed transition is interpreted as 2 A 1 → 2 B 1 resulting from a π → n excitation.





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