1998
DOI: 10.1070/pu1998v041n04abeh000384
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Vibrational relaxation of excimers

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Cited by 16 publications
(6 citation statements)
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“…The high excitation effi ciency of higher energy states (C 2 Π 1/2 and D 2 Π 3/2 ) of mercury monobromide molecules, as well as the dependence of the HgBr* exciplex radiation power on the sulfur hexafluoride partial pressure (the radiation power increases many times) [13], suggests that mole cules in these energy states occupy the state B 2 of The run of the dependence of the HgBr* exciplex radiation power on the nitrogen partial pressure (Fig. 3) depends on the (i) electron concentration, which increases with nitrogen partial pressure in the mixture; (ii) fraction of the discharge energy that is spent on heating the working mixture; (iii) electron mean energy; (iv) rate of dissociative excitation of the HgBr* exciplex by electrons and nitrogen molecules excited into the metastable states A 3 and B 3 Π g ; (v) popula tion of these states, which increases owing to the relax ation of the populations of higher vibrational levels in collisions with working mixture components, and (vi) quenching of the HgBr* exciplex by molecules of mer cury dibromide, sulfur hexafluoride, and nitrogen and also by atoms of helium [30][31][32][33][34][35]. A rise in the nitrogen partial pressure causes a decrease in parameter E/N and, accordingly, leads to an increase in the discharge power specific losses due to elastic scattering by atoms and molecules (heating of the mixture) [36].…”
Section: Discussion Of Resultsmentioning
confidence: 99%
“…The high excitation effi ciency of higher energy states (C 2 Π 1/2 and D 2 Π 3/2 ) of mercury monobromide molecules, as well as the dependence of the HgBr* exciplex radiation power on the sulfur hexafluoride partial pressure (the radiation power increases many times) [13], suggests that mole cules in these energy states occupy the state B 2 of The run of the dependence of the HgBr* exciplex radiation power on the nitrogen partial pressure (Fig. 3) depends on the (i) electron concentration, which increases with nitrogen partial pressure in the mixture; (ii) fraction of the discharge energy that is spent on heating the working mixture; (iii) electron mean energy; (iv) rate of dissociative excitation of the HgBr* exciplex by electrons and nitrogen molecules excited into the metastable states A 3 and B 3 Π g ; (v) popula tion of these states, which increases owing to the relax ation of the populations of higher vibrational levels in collisions with working mixture components, and (vi) quenching of the HgBr* exciplex by molecules of mer cury dibromide, sulfur hexafluoride, and nitrogen and also by atoms of helium [30][31][32][33][34][35]. A rise in the nitrogen partial pressure causes a decrease in parameter E/N and, accordingly, leads to an increase in the discharge power specific losses due to elastic scattering by atoms and molecules (heating of the mixture) [36].…”
Section: Discussion Of Resultsmentioning
confidence: 99%
“…In [15], interaction of excimers with plasma electrons was studied in the framework of the Bethe-Born approximation of the scattering theory. The following rate constant of an electron-induced molecular transition was obtained [15,16]:…”
Section: Molecular Transitions In Collisions Of Molecules With Plasma...mentioning
confidence: 99%
“…Earlier, this reaction was included in a kinetic model of the HgBr avalanche discharge laser [14]. A formula for the rate constant of a molecular transition induced by collisions of the molecule with plasma electrons was derived in our previous work [15,16]. This formula was used in a kinetic study of a HgBr lamp excited by single current pulses [17].…”
Section: Introductionmentioning
confidence: 99%
“…In the literature there are almost no data which would allow to strictly determine a dependence of the relaxation process rates on vibrational structure. Especially, this concerns the rates of collision-induced deactivation of excimer molecules [45].…”
Section: Xe Concentration Effect On the Intensity Of Emission From Himentioning
confidence: 99%
“…The lower levels (V =0, 1 i 2) we will place in the second band. The first band width is largerthan a vibrational quantum, and the VT relaxation in it can be considered as diffusion in a quasicontinuous energy space [44,45]. The time of diffusion of molecules in the first band let us denote as t and a total time of thermalization of the vibrational subsystem in the second band as t2.…”
Section: Spectral Regimes Of the Xef Molecule Lasingmentioning
confidence: 99%