Vibrational Distribution of N2(B3Πg) Produced from Dissociative Recombination of N2O+in a Helium Flowing Afterglow

2000 ◽  
Vol 29 (6) ◽  
pp. 592-593 ◽  
Author(s):  
Masaharu Tsuji ◽  
Takeshi Tanoue ◽  
Yuki Tanaka ◽  
Yukio Nishimura
1992 ◽  
Vol 194 (4-6) ◽  
pp. 263-267 ◽  
Author(s):  
H. Abouelaziz ◽  
J.L. Queffelec ◽  
C. Rebrion ◽  
B.R. Rowe ◽  
J.C. Gomet ◽  
...  

2004 ◽  
Vol 108 (32) ◽  
pp. 6704-6708 ◽  
Author(s):  
Jason L. McLain ◽  
Viktoriya Poterya ◽  
Christopher D. Molek ◽  
Lucia M. Babcock ◽  
Nigel G. Adams

2016 ◽  
Vol 145 (24) ◽  
pp. 244312 ◽  
Author(s):  
Justin P. Wiens ◽  
Thomas M. Miller ◽  
Nicholas S. Shuman ◽  
Albert A. Viggiano

1987 ◽  
Vol 7 (5-6) ◽  
pp. 333-341 ◽  
Author(s):  
Masaharu Tsuji ◽  
Ichiro Nagano ◽  
Nobuaki Nishiyama ◽  
Hiroshi Sekiya ◽  
Yukio Nishimura

Thermal energy reactions of C+(2P) and C(1D,1S) with CH3OH, C2H5OH, n-C3H7OH and i-C3H7OH to give CH(X2Π) radicals have been investigated by observing laser-induced fluorescence (LIF) spectra of CH(A—X) in a flowing afterglow. In the hydride ion abstraction by C+(2P), only CH3OH exhibited the CH(A—X) LIF spectrum with a vibrational distribution of 1.0 : 0.62 for v″ = 0 and 1, respectively. On the other hand, the CH(A—X) LIF spectra exclusively from v″ = 0 were observed in the reactions of C(1D,1S) with all alcohols studied. By isotopic substitution for CH3OH it was shown that the CH(X) radicals arise from the selective attack on the methyl site in the reactions of C+(2P) and C(1D,1S) with methanol.


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