Kalogerakis Konstantinos S, Copeland Richard A, Slanger Tom G
Molecular Physics Laboratory, SRI International, Menlo Park, California 94025, USA.
J Chem Phys. 2005 Jul 22;123(4):044309. doi: 10.1063/1.1982788.
Vibrational relaxation of O2(X 3sigma(g)-, upsilon=2,3) by O2 molecules is studied via a two-laser approach. Laser radiation at 266 nm photodissociates ozone in a mixture of molecular oxygen and ozone. The photolysis step produces vibrationally excited O2(a 1delta(g)) that is rapidly converted to O2(X 3sigma(g)-, upsilon=2,3) in a near-resonant adiabatic electronic energy-transfer process involving collisions with ground-state O2. The output of a tunable 193-nm ArF laser monitors the temporal evolution of the O2(X 3sigma(g)-, upsilon=2,3) population via laser-induced fluorescence detected near 360 nm. The rate coefficients for the vibrational relaxation of O2(X 3sigma(g)-, upsilon=2,3) in collision with O2 are 2.0(-0.4)(+0.6) x 10(-13) cm3 s(-1) and (2.6+/-0.4) x 10(-13) cm3 s(-1), respectively. These rate coefficients agree well with other experimental work but are significantly larger than those produced by various semiclassical theoretical calculations.
通过双激光方法研究了O₂分子对O₂(X³σg⁻, υ = 2,3)的振动弛豫。266 nm的激光辐射使分子氧和臭氧混合物中的臭氧发生光解。光解步骤产生振动激发的O₂(a¹Δg),其在涉及与基态O₂碰撞的近共振绝热电子能量转移过程中迅速转化为O₂(X³σg⁻, υ = 2,3)。可调谐193 nm ArF激光的输出通过在360 nm附近检测到的激光诱导荧光监测O₂(X³σg⁻, υ = 2,3)布居的时间演化。O₂(X³σg⁻, υ = 2,3)与O₂碰撞时的振动弛豫速率系数分别为2.0(-0.4)(+0.6)×10⁻¹³ cm³ s⁻¹和(2.6±0.4)×10⁻¹³ cm³ s⁻¹。这些速率系数与其他实验工作吻合良好,但明显大于各种半经典理论计算得出的结果。