Abstract

The time dependence of luminescence in liquid argon and xenon has been studied for electron, $\ensuremath{\alpha}$-particle, and fission-fragment excitation. The lifetimes of low excited molecular states ($^{1}\ensuremath{\Sigma}_{u}^{+}$ and $^{3}\ensuremath{\Sigma}_{u}^{+}$) do not depend on the density of excited species while the intensity ratio of $^{1}\ensuremath{\Sigma}_{u}^{+}$ to $^{3}\ensuremath{\Sigma}_{u}^{+}$ is found to be larger at higher deposited energy density. The lifetimes obtained for the $^{1}\ensuremath{\Sigma}_{u}^{+}$ and $^{3}\ensuremath{\Sigma}_{u}^{+}$ states are 7.0 \ifmmode\pm\else\textpm\fi{} 1.0 nsec and 1.6 \ifmmode\pm\else\textpm\fi{} 0.1 \ensuremath{\mu}sec, respectively, in liquid argon, and 4.3 \ifmmode\pm\else\textpm\fi{} 0.6 and 22.0 \ifmmode\pm\else\textpm\fi{} 2.0 nsec, respectively, in liquid xenon. The mechanism of quenching of luminescence at a high density of excited species in liquid argon and xenon is discussed.

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