新疆大学物理科学与技术学院,新疆大学物理科学与技术学院,新疆大学物理科学与技术学院,新疆大学物理科学与技术学院 新疆乌鲁木齐830046,西安交通大学理学院,陕西西安710049,新疆乌鲁木齐830046,西安交通大学理学院,陕西西安710049,新疆乌鲁木齐830046,新疆,乌鲁木齐,830046
纸质出版:2007
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[1]刘静,王淑英,戴康,等.Rb(5P_J)与He的碰撞精细结构混合和猝灭(英文)[J].新疆大学学报(自然科学版),2007,No.108(04):413-417.
刘静, 王淑英, 戴康, et al. Rb(5PJ)与He的碰撞精细结构混合和猝灭(英文)[J]. Journal of Xinjiang University (Natural Science Edition in Chinese and English), 2007, 108(4): 413-417.
应用激光吸收和荧光方法
测量了Rb(5PJ)态与He原子碰撞的精细结构转移和碰撞猝灭截面.Rb原子被激光激发到5P3/2态
将与泵浦激光束反向平行的检测激光束调到5PJ→7S1/2的跃迁
测量5PJ激发态原子的密度及空间分布
由此计算了5PJ→5S的有效辐射率.在T=340K和He密度0.5×1017 关键词: 碰撞能量转移; 荧光; 截面; 铷; 氮气; Abstract: Applying the cw laser absorption and fluorescence method
the cross sections for the fine structure mixing and quenching of the Rb(5PJ) state
induced by collisions with He atoms have been measured
Rubidium atoms were optically excited to 5 P3/2states.The excited atom density and spatial distribution were mapped by monitoring the absorption of a counterpropagating single mode laser beam
tuned to the 5PJ→ 7S1/2 transitions.Transmission factors were calculated for the 5PJ→ 5S transitions.The fluorescence intensity I795 of the sensitized 5P1/2→ 5S1/2emission was measured as a function of He density in the range 0.5×1017< N <4× 1017cm-3at constant temperature T = 340 K.It was found that the quantity N/ I795 exhibited a parabolic dependence on N
confirming that the quenching of the 5PJ states is due to collision with He atoms
not due to Rb ground state atoms.The coefficients of the second-order polynomial fitted through the measured date yielded the cross sectionsσ3/2→1/2=(1.84± 0.61)× 10-17cm2 andσD=(1.07± 0.30)× 10-17cm2 for the 5PJfine-structure mixing and quenching
respectively
due to collision with He atoms. KeyWords: collision energy transfer; fluorescence; cross sections; Rubidium atoms; He atoms;
Applying the cw laser absorption and fluorescence method
the cross sections for the fine structure mixing and quenching of the Rb(5PJ) state
induced by collisions with He atoms have been measured
Rubidium atoms were optically excited to 5 P3/2states.The excited atom density and spatial distribution were mapped by monitoring the absorption of a counterpropagating single mode laser beam
tuned to the 5PJ→ 7S1/2 transitions.Transmission factors were calculated for the 5PJ→ 5S transitions.The fluorescence intensity I795 of the sensitized 5P1/2→ 5S1/2emission was measured as a function of He density in the range 0.5×1017< N <4× 1017cm-3at constant temperature T = 340 K.It was found that the quantity N/ I795 exhibited a parabolic dependence on N
confirming that the quenching of the 5PJ states is due to collision with He atoms
not due to Rb ground state atoms.The coefficients of the second-order polynomial fitted through the measured date yielded the cross sectionsσ3/2→1/2=(1.84± 0.61)× 10-17cm2 andσD=(1.07± 0.30)× 10-17cm2 for the 5PJfine-structure mixing and quenching
respectively
due to collision with He atoms.
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Shen Y F,Dai K,Mu B X,et al.Resonant Reaction in Rb-Cs Vapour Mixture Rb(5P1/2)+Cs(6P3/2)→Cs(8S1/2)+Rb(5S1/2)[J].Chin Phys Lett,2006,23:1173.
Pitre F S C Bruce,Rae A G A,Krause L.Sensitized fluorescence in vapors of alkali metals VI.Energy transfer incollisions between rubidium and inert gas atoms[J].Can J Phys,1966,44:731.
Jabbour Z J,Namiotka R K,Huennehens J.Energy-pooling collisions in cesium:6PJ+6PJ6S+(nl=7 P,6D,8S,4F)[J].Phys Rev,1996:A54(2):1372.
Niemax K,Movre M,Pichler G.Near-wing asymmetries of the self-broadened first Rb and Cs resonance lines[J].JPhys,1979,B12(21):3503.
Davies J T,Vaughan J M.A New tabulation of the voigt profile[J].Astrophysics J,1963,137:1302.
Gallaghor A.Rubidium and cesium excitation tramsfer in nearly adiabatic collisions with inert gases[J].Phys Rev,1968,172:88.
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