A. Francis et al., Collisional deactivation of two-photon-excited Ar (4p; J = 0, 2) states byH-2 and several hydrocarbon and fluorine containing molecules, EPJ-APPL PH, 4(3), 1998, pp. 239-242
The quenching rate constants of argon atoms in the 4p'[1/2](0)-(2p(1)), 4p[
1/2](0)-(2p(5)), 4p[3/2](2)-(2p(6)) and 4p[5/2](2)-(2p(8)) states, the uppe
r levels of the 750.4, 751.5, 763.5 and 801.5 nm lines respectively, by H-2
, CH4, C2H2, C2H4, C2H6, CF4, CHF3 and SF6 have been determined. Argon atom
s at room temperature are two-photon excited in the 184-190 nm range, and t
he decay time of the fluorescence emission is measured in the presence of v
arious reagents. With H-2, the collisional quenching rate coefficients of A
r(2p(1)), Ar(2p(5)), Ar(2p(6)) and Ar(2p(8)) are 0.27, 4.1, 6.8 and 5.4 x 1
0(-10) cm(3)s-(1), respectively. Therefore, in hydrogen rich plasmas, the 7
50.4 nm line of argon is the best suited for actinometry measurements. For
the other studied molecules, the quenching rates range between 1.6 and 11 x
10(-10) cm(3)s(-1). For a correct estimation of the relative density of tr
ansient species in plasma by the actinometry technique, it is recommended t
o consider the collisional quenching of the upper states of the optical emi
ssion lines used.