窒素分子による準安定アルゴン原子の失活とN<SUB>2</SUB> (<I>C</I><SUP>3</SUP><I>II<SUB>u</SUB></I>) 状態の罪平衡回転準位分布
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The excited levels argon (Ar<SUP>*</SUP>;1 s<SUB>5</SUB>, 1 s<SUB>4</SUB>, 1 s<SUB>3</SUB> and 1 s<SUB>2</SUB>) are populated by means of a DC discharge in argon-nitrogen mixtures. The densities of Ar<SUP>*</SUP> (<I>nj</I>;<I>j</I>=5, 4, 3, 2) are measured by optical absorption techniques.The deactivation cross-sections (<I>Q<SUB>jo</SUB></I>) of Ar<SUP>*</SUP> (1s<SUB><I>j</I></SUB>) by N<SUB>2</SUB> are determined from the dependence of <I>n<SUB>j</SUB></I> on nitrogen fraction and are 0.75±0.10, 2.2±1.1, 0.32± 0.06 and <3.3 Å<SUP>2</SUP> for the 1 s<SUB>5</SUB>, 1 s<SUB>4</SUB>, 1 s<SUB>3</SUB> and 1 s<SUB>2</SUB> levels respectively.<BR>The (0, 2) band of N<SUB>2</SUB> second positive system is observed at the same time and it is clarified that Ar<SUP>*</SUP> excites the N<SUB>2</SUB> (C<SUP>3</SUP><I>II<SUB>u</SUB></I>), υ=0 level which is characteristic of the nonequilibrium rotational populations such as the enhanced structure and alternating population.The ratios of the excitation rates of the N<SUB>2</SUB> (C<SUP>3</SUP><I>II<SUB>u</SUB></I>), υ=0 level by electrons and Ar<SUP>*</SUP> are obtained from analysis of the nonequilibrium rotational populations for different nitrogen fractions, and explained by considering <I>n<SUB>j</SUB></I> and <I>Q<SUB>jo</SUB></I>.The cross-section of rotational relaxation (30±10 Å<SUP>2</SUP>) is also obtained from study of the dependence of alternating populations upon the pressure.<BR>The collisional mechanisms between Ar<SUP>*</SUP> and N<SUB>2</SUB> are discussed mainly on the basis of the one-step mechanism consisted of the ArN<SUB>2</SUB><SUP>*</SUP> complex proposed by Setser and Stedman.
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