Johnson Jeremy A, Kim Kilyoung, Mayhew Maurine, Mitchell Deborah G, Sevy Eric T
Department of Chemistry and Biochemistry, Brigham Young University, Provo, Utah 84602, USA.
J Phys Chem A. 2008 Mar 27;112(12):2543-52. doi: 10.1021/jp076543d. Epub 2008 Mar 6.
Relaxation of highly vibrationally excited pyridine (C5NH5) by collisions with carbon dioxide has been investigated using diode laser transient absorption spectroscopy. Vibrationally hot pyridine (E' = 40,660 cm(-1)) was prepared by 248 nm excimer laser excitation followed by rapid radiationless relaxation to the ground electronic state. Pyridine then collides with CO2, populating the high rotational CO2 states with large amounts of translational energy. The CO2 nascent rotational population distribution of the high-J (J = 58-80) tail of the 00(0)0 state was probed at short times following the excimer laser pulse to measure rate constants and probabilities for collisions populating these CO2 rotational states. Doppler spectroscopy was used to measure the CO2 recoil velocity distribution for J = 58-80 of the 00(0)0 state. The energy-transfer distribution function, P(E,E'), from E' - E approximately 1300-7000 cm(-1) was obtained by re-sorting the state-indexed energy-transfer probabilities as a function of DeltaE. P(E,E') is fit to an exponential or biexponential function to determine the average energy transferred in a single collision between pyridine and CO2. Also obtained are fit parameters that can be compared to previously studied systems (pyrazine, C6F6, methylpyrazine, and pyrimidine/CO2). Although the rotational and translational temperatures that describe pyridine/CO2 energy transfer are similar to previous systems, the energy-transfer probabilities are much smaller. P(E,E') fit parameters for pyridine/CO2 and the four previously studied systems are compared to various donor molecular properties. Finally, P(E,E') is analyzed in the context of two models, one indicating that P(E,E') shape is primarily determined by the low-frequency out-of-plane donor vibrational modes, and the other that indicates that P(E,E') shape can be determined from how the donor molecule final density of states changes with DeltaE.
利用二极管激光瞬态吸收光谱研究了高振动态激发的吡啶(C₅NH₅)与二氧化碳碰撞时的弛豫过程。通过248nm准分子激光激发制备出振动态热的吡啶(E' = 40,660 cm⁻¹),随后快速无辐射弛豫至基电子态。吡啶接着与二氧化碳碰撞,使高转动的二氧化碳态填充大量平动能。在准分子激光脉冲后的短时间内探测00(0)0态高J(J = 58 - 80)尾部的二氧化碳初始转动布居分布,以测量填充这些二氧化碳转动态的碰撞速率常数和概率。利用多普勒光谱测量00(0)0态J = 58 - 80的二氧化碳反冲速度分布。通过将按态索引的能量转移概率重新整理为ΔE的函数得到能量转移分布函数P(E,E'),其范围为E' - E约1300 - 7000 cm⁻¹。将P(E,E')拟合为指数或双指数函数,以确定吡啶与二氧化碳单次碰撞中转移的平均能量。还得到了可与先前研究的体系(吡嗪、C₆F₆、甲基吡嗪和嘧啶/二氧化碳)进行比较的拟合参数。尽管描述吡啶/二氧化碳能量转移的转动和平动温度与先前体系相似,但能量转移概率要小得多。将吡啶/二氧化碳和四个先前研究体系的P(E,E')拟合参数与各种供体分子性质进行比较。最后,在两种模型的背景下分析P(E,E'),一种模型表明P(E,E')形状主要由低频面外供体振动模式决定,另一种模型表明P(E,E')形状可由供体分子终态密度随ΔE的变化来确定。