S. Bockel et al., OPTICAL DIAGNOSTICS OF ACTIVE SPECIES IN N-2 MICROWAVE FLOWING POSTDISCHARGES, Surface & coatings technology, 74-5(1-3), 1995, pp. 474-478
The nitrogen atom density is determined from NO titration and from the
N-2 first-positive-band intensity. The main kinetic reactions which p
roduce the N-2 first-positive-band emission in the afterglow are the f
ollowing: [GRAPHICS] in an early afterglow at times 10(-3)-10(-2)s and
N + N + N-2 --> N-2(B, upsilon') + N-2 in the full afterglow period (
10(-3)-10(-1)s). From the N-2(B, upsilon'-A, upsilon '') first-positiv
e-band intensity, parts of the above reactions have been established a
long a 2.45 GHz, 120 W N-2 flowing post-discharge at 5-130 hPa gas pre
ssure and at 0.2-1 standard 1 min(-1) flow rate. It has been found tha
t the NO titration method is only available in the late afterglow wher
e the second reaction is dominant. By discriminating the second reacti
on from the first reaction, the first-positive-band intensity allows t
he N atom density determination in the post-discharge, along a larger
domain than with NO titration including the end of the early afterglow
. Furthermore, the first reactions contribute to produce highly excite
d levels up to N-2(B, upsilon' = 17, 18) whose vibrational distributio
n is given in the present paper. These levels, whose N-2(B, upsilon' >
13-15) states are autodissociative states are not created by the seco
nd reaction. Consequently, this is also a second method for specifying
the afterglow parts where the above reactions are the dominant kineti
c processes.