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Appendix
N2 pressure
(a) 0 mTorr
Cl*
B-X
D-X
ArCl
B-X
N2 pressure
(a) 0 mTorr
C-A
ArCl
D-X
C-A
Cl*
(b) 21 mTorr
(b) 5 mTorr
(c) 47 mTorr
(d) 70 mTorr
(c) 14 mTorr
(e) 93 mTorr
(f) 140 mTorr
120
140
160
180
200
220
(d) 19 mTorr
Wavelength (nm)
Fig. A1. Effects of N2 addition to the
emission spectra of ArCl* resulting from the
Ar+(2P1/2,3/2)/C6F5Cl- reaction in the Ar
afterglow.
120
140
160
180
200
220
Wavelength (nm)
Fig. A2. Effects of N2 addition to the emission
spectra of ArCl* resulting from the
Ar+(2P1/2,3/2)/C6F5Cl- reaction in the He
afterglow.
Spin-orbit state selectivity for RgCl(B,C,D) excimers produced from recombination reactions of Rg+ with C6F5Cl-
Rg+(2P3/2) + X2-(2Σu+)
Rg+(2P1/2) + X2-(2Σu+)
Potential energy
24
01,0+
Rg(3P0) + X2(1Σg+)
2,1,0Rg(3P2)
Rg(3P1) + X2(1Σg+)
+ X2(1Σg+)
2,1
Rg + X2
R(Rg―X2)
Fig. A3. Correlation diagram of the diabatic potentials for
the Rg(3P0,2)/X2 and Rg+(2P1/2,3/2)/X2- reactions in collinear
geometry.5) The states with Rg+(2P1/2) ion-core configuration
are shown by dashed lines. The dark circles show positions
of expected strong interactions of the diabatic potentials. The
only Ω = 1/2 components correlating to X(2P3/2) have been
included in the drawing because they are more important
than Ω = 3/2 components.
...