首页> 外文学位 >Dynamics of rovibrational energy transfer from excited molecular iodine: New crossed beam studies.
【24h】

Dynamics of rovibrational energy transfer from excited molecular iodine: New crossed beam studies.

机译:激发分子碘传递振动能量的动力学:新的交叉束研究。

获取原文
获取原文并翻译 | 示例

摘要

Rovibrational inelastic scattering has been studied for the collisions between helium and excited molecular iodine (I{dollar}sb2{dollar}) in a crossed beam apparatus. I{dollar}sb2{dollar} was initially prepared in two vibrational states, {dollar}upsilonprime{dollar} = 15 and 35, in the B O{dollar}sb{lcub}rm u{rcub}sp +{dollar} electronic state. Dispersed single vibrational level fluorescence spectra revealed the vibrational inelastic scattering. The collision energy (Ecm) was varied from 35meV to 190meV. Vibrational state changes up to {dollar}vert Deltaupsilonvert{dollar} = 6 in {dollar}upsilonprime{dollar} = 35 and {dollar}vert Deltaupsilonvert{dollar} = 3 in {dollar}upsilonprime{dollar} = 15 were observed. Nearly 200 relative vibrational state-to-state inelastic scattering cross sections were measured.; At each Ecm, all the cross sections for both {dollar}upsilonprime{dollar} = 15 and 35 can be fitted by a single exponential function {dollar}sigma propto{dollar} exp(-{dollar}vert Deltarm Evert/beta{dollar}). At high Ecm, {dollar}betasb{lcub}rm Vto T{rcub}{dollar} is equal to {dollar}betasb{lcub}rm Tto V{rcub}{dollar}. At low ECM, {dollar}betasb{lcub}rm Vto T{rcub}{dollar} is larger than {dollar}betasb{lcub}rm Tto V{rcub}{dollar}. However, all {dollar}beta{dollar}'s are linear functions of Ecm. Also the cross sections for the {dollar}Deltaupsilon{dollar} = {dollar}pm{dollar}1 scattering are nearly independent of Ecm. Considering that the collisions are not adiabatic, these results are not consistent with the well-known Landau-Teller theory.; Using the empirical dependence of the cross sections on Ecm, we calculated the thermal rate constants. The calculation at 300K agrees with the bulb experiment for V {dollar}to{dollar} T but not for T {dollar}to{dollar} V transitions. The calculation also shows that the bulb energy transfer is mainly induced by collisions with velocities {dollar}sim{dollar}2 times larger than the most probable velocity.; From the cross sections, mean energy transfer per vibrationally inelastic collision, {dollar}langle Deltarm Erangle{dollar}, was also obtained. The results show that {dollar}langle Deltarm Erangle{dollar} increases linearly with Ecm and levels off to near-zero at high collision energy. At low Ecm, {dollar}langle Deltarm Erangle{dollar} in {dollar}upsilonprime{dollar} = 15 is larger than that in {dollar}upsilonprime{dollar} = 35.; The average rotational energy transfered increases almost linearly with Ecm but is small, only {dollar}sim{dollar}2% of the Ecm. This is a direct result of angular momentum conservation.; Classical trajectory calculations were carried out with an available program. Using an exponential interaction potential, the calculated and experimental cross sections agree fairly well. The calculations reveal that the exponential {dollar}vert Deltarm Evert{dollar} dependence of the cross sections is a result of 3-dimensional averaging.
机译:已经研究了在横梁装置中氦与激发的分子碘(I {dollar} sb2 {dollar})之间碰撞的振动振动非弹性散射。 I {dollar} sb2 {dollar}最初是在BO {dollar} sb {lcub} rm u {rcub} sp + {dollar}电子状态的两个振动状态下准备的,分别为{dollar} upsilonprime {dollar} = 15和35。 。分散的单个振动级荧光光谱揭示了振动非弹性散射。碰撞能量(Ecm)从35meV变化到190meV。观察到{dollar} upsilonprime {dollar} = 35中的振动状态变化高达{dollar} vert Deltaupsilonvert {dollar} = 6,并且在{dollar} upsilonprime {dollar} = 15中观察到{dollar} vert Deltaupsilonvert {dollar} = 3。测量了近200个相对振动状态间非弹性散射截面。在每个Ecm处,{dollar} upsilonprime {dollar} = 15和35的所有横截面都可以通过单个指数函数{dollar} sigma propto {dollar} exp(-{dollar} vert Deltarm Evert / beta {dollar)进行拟合}。在高Ecm时,{dols} betasb {lcub} rm Tto V {r​​cub} {dollar}等于{dollar} betasb {lcub} rm Tto V {r​​cub} {dollar}。在低ECM时,{dols} betasb {lcub} rm Tto V {r​​cub} {dollar}大于{dollar} betasb {lcub} rm Tto V {r​​cub} {dollar}。但是,所有{beta} {dollar}都是Ecm的线性函数。同样,{美元} Deltaupsilon {美元} = {美元} pm {美元} 1散射的横截面几乎与Ecm无关。考虑到碰撞不是绝热的,这​​些结果与著名的Landau-Teller理论不一致。使用横截面对Ecm的经验依赖性,我们计算了热速率常数。在300K时的计算与V {dollar}到{dollar} T的灯泡实验相吻合,但与T {dollar}到{dollar} V过渡的灯泡实验吻合。计算还表明,灯泡的能量传递主要是由与最可能的速度大2倍的速度碰撞引起的。从横截面中,还获得了每个振动非弹性碰撞的平均能量传递,即ΔDeltaDeltarm Erangle。结果表明,{美元}长三角ΔErangle{美元}随着Ecm线性增加,在高碰撞能量下趋近于零。在低Ecm时,{dollar} upsilonprime {dollar} = 15中的{dollar} l Deltarm Erangle {dollar}大于{dollar} upsilonprime {dollar} = 35中的{Delta}。传递的平均旋转能量几乎随Ecm线性增加,但很小,仅为Ecm的2%。这是角动量守恒的直接结果。经典轨迹计算是使用可用程序进行的。使用指数相互作用势,计算得出的横截面和实验横截面相当吻合。计算结果表明,横截面的指数{dolal} vert Deltarm Evert {dollar}依赖性是3维平均的结果。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号