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作 者:周冬冬[1] 王大贵[1] 王雪燕[1] 穆尼赛[1] 戴康[1] 沈异凡[1]
机构地区:[1]新疆大学物理科学与技术学院,乌鲁木齐830046
出 处:《激光杂志》2010年第1期28-29,共2页Laser Journal
基 金:国家自然科学基金资助项目(10664003)
摘 要:Cs蒸气置于十字交叉加热炉中,充入不同气压的H2,激光双光子激发Cs原子至6D3/2态,利用原子荧光光谱方法,研究了H2诱导6DJ→7PJ,的碰撞能量转移。测量不同氢气密度下直接6D3/2→6P3/2和敏化6D5/2→6P3/2,7P3/2→6S1/2和7P1/2→6S1/2的时间积分荧光强度,利用四粒子的速率方程分析,得到了6D3/2→7P3/2,6D3/2→7P1/2,6D5/2→7P3/2和6D5/2→7P1/2碰撞转移截面分别为(3.1±0.8)×10-16,(1.7±0.4)×10-16,(1.5±0.4)×10-16,(1.3±0.3)×10-16cm2。7PJ′态的猝灭截面分别为(2.5±0.6)×10-16cm2(对7P3/2)和(4.0±1.0)×10-16cm2(对7P1/2),它们主要是通过Cs(7PJ′)+H2→CsH+H反应产生的,而反应的相对活动性顺序为7P1/2>7P3/2。Cs vapor was created in a resistively heated,cross-shaped stainless-steel heat-pipe oven with quartz windows.H2 gas filled in the cell for use both as a buffer gas and as a reaction partner.Cs atoms were excited to 6D3/2 state by two-photon absorption.The 7P1/2 and 7P3/2 were populated by the radiative and collisional 6DJ→7PJ′ transition.The cross sections for 6DJ7PJ′ transfer induced by collision with H2 molecules have been determined using methods of atomic fluorescence.The resulting fluorescence included a direct component emitted in the decay of the optically excited state and sensitive component arising from collisionally populated states.The time-integrated fluorescence intensities for atomic transitions 6D5/2→6P3/2,6D3/2→6P3/2,7P3/2→6S1/2 and 7P1/2→6S1/2 were measured at the defferent H2 densities.The relative time-integrated population densities were obtained as a function of H2 densities.By the set of the rate equations,the cross-sections have been determined to be σ6D3/27P3/2=(3.1±0.8)×10^-16cm^2,σ6D3/27P1/2=(1.7±0.4)×10^-16cm^2,σ6D5/27P3/2=(1.5±0.4)×10^-16cm^2 and σ6D5/27P1/2=(1.3±0.3)×10^-16 cm2.The cross sections for quenching of 7PJ′ by H2 are(2.5±0.6)×10^-16 cm^2(for 7P3/2) and(4.0±1.0)×10^-16 cm2(for 7P1/2).Evidence suggests that the substantial fraction of quenching cross section is reactive.The relative reactivity with H2 is an order 7P1/27P3/2.
关 键 词:激光光谱 碰撞能量转移 原子荧光:截面 Cs*+H2
分 类 号:O562.3[理学—原子与分子物理] O562.4[理学—物理]
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