Potter A B, Wei J, Reisler H
Department of Chemistry, University of Southern California, Los Angeles, California 90089-0482, USA.
J Phys Chem B. 2005 May 5;109(17):8407-14. doi: 10.1021/jp046226w.
Photofragment yield spectra and NO(X(2)Pi(1/2,3/2); v = 1, 2, 3) product vibrational, rotational, and spin-orbit state distributions were measured following NO dimer excitation in the 4000-7400 cm(-1) region in a molecular beam. Photofragment yield spectra were obtained by monitoring NO(X(2)Pi; v = 1, 2, 3) dissociation products via resonance-enhanced multiphoton ionization. New bands that include the symmetric nu(1) and asymmetric nu(5) NO stretch modes were observed and assigned as 3nu(5), 2nu(1) + nu(5), nu(1) + 3nu(5), and 3nu(1) + nu(5). Dissociation occurs primarily via Deltav = -1 processes with vibrational energy confined preferentially to one of the two NO fragments. The vibrationally excited fragments are born with less rotational energy than predicted statistically, and fragments formed via Deltav = -2 processes have a higher rotational temperature than those produced via Deltav = -1 processes. The rotational excitation likely derives from the transformation of low-lying bending and torsional vibrational levels in the dimer into product rotational states. The NO spin-orbit state distribution reveals a slight preference for the ground (2)Pi(1/2) state, and in analogy with previous results, it is suggested that the predominant channel is X(2)Pi(1/2) + X(2)Pi(3/2). It is suggested that the long-range potential in the N-N coordinate is the locus of nonadiabatic transitions to electronic states correlating with excited product spin-orbit states. No evidence of direct excitation to electronic states whose vertical energies lie in the investigated energy region is obtained.
在分子束中,于4000 - 7400 cm⁻¹区域对NO二聚体进行激发后,测量了光碎片产率光谱以及NO(X²Π₁/₂,₃/₂; v = 1, 2, 3)产物的振动、转动和自旋 - 轨道态分布。通过共振增强多光子电离监测NO(X²Π; v = 1, 2, 3)解离产物来获得光碎片产率光谱。观察到了包括对称ν₁和不对称ν₅ NO伸缩模式的新谱带,并将其归属为3ν₅、2ν₁ + ν₅、ν₁ + 3ν₅和3ν₁ + ν₅。解离主要通过Δv = -1过程发生,振动能量优先局限于两个NO碎片之一。振动激发的碎片产生时的转动能量比统计预测的要少,并且通过Δv = -2过程形成的碎片比通过Δv = -1过程产生的碎片具有更高的转动温度。转动激发可能源于二聚体中低阶弯曲和扭转振动能级向产物转动态的转变。NO自旋 - 轨道态分布显示出对基态(²Π₁/₂)的轻微偏好,并且与先前的结果类似,表明主要通道是X²Π₁/₂ + X²Π₃/₂。有人提出,N - N坐标中的长程势是向与激发产物自旋 - 轨道态相关的电子态进行非绝热跃迁的场所。未获得直接激发到垂直能量位于所研究能量区域的电子态的证据。