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True quantum state-to-quantum state chemistry: Experimental determination of the transition dipole matrix.

机译:真正的量子态到量子态化学:跃迁偶极子矩阵的实验确定。

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The dynamics of photodissociation reactions of 2 different systems were studied in detail. For both systems the initial {dollar}vert JKMrangle{dollar} rotational state was selected using an electrostatic hexapole "filter." Selection of the initial reactant quantum state coupled with state-selective detection of the photoproducts allows determination of the greatest amount of information possible for a chemical reaction. This in turn allows determination of the molecule-specific transition dipole matrix elements (T-matrix) which contains all of the dynamical information for the chemical reaction.; In the first experiment a beam of deuterated methyl iodide, {dollar}rm CDsb3I,{dollar} seeded in xenon (5-10%) was focused by the electrostatic hexapole into the {dollar}vert 111rangle{dollar} rotational state of the vibrationless ground electronic state, {dollar}tilde X sp1Asb1.{dollar} The state-selected molecules were then photodissociated in the A band by a laser at 266 nm. The population and alignment (second and fourth rank spherical moments) of several of the individual rotational states (low total angular momentum, {dollar}Jle 2){dollar} of the methyl photofragment were then measured via (2+1) REMPI via the {dollar}rm 3psp2Asbsp{lcub}2{rcub}{lcub}primeprime{rcub}gets 2psp2Asbsp{lcub}2{rcub}{lcub}primeprime{rcub}{dollar} electronic transition. Quantum state-specific angular distributions of the methyl photofragments were measured via time-of-flight (TOF) spectroscopy. In addition, from these measurements of the detailed cross sections (both integral and differential), elements of the T-matrix were calculated, representing the highest level of detail possible for a photodissociative reaction.; In the second experiment a beam of nitrosyl chloride (NOCl) seeded in argon (10-50%) was state selected by the electrostatic hexapole and then photodissociated in the B band at {dollar}{lcub}sim{rcub}355{dollar} nm. The angular distribution, state population, and rotational alignment of several product nitric oxide (NO) rotational states (high total angular momentum, {dollar}Jge 39.5){dollar} were determined. The product NO rotational distribution was quite hot, with a peak in the distribution much higher than {dollar}J = 30{dollar} with a propensity for {dollar}{lcub}bf J{rcub}{dollar} (total angular momentum) to be oriented perpendicular to the laboratory Z-axis. From measurements of both the angle-integrated alignment moments and the photofragment angular distributions, possible T-matrix amplitudes and phases were estimated.
机译:详细研究了两种不同系统的光解离反应动力学。对于这两个系统,使用静电六极杆“滤波器”来选择初始{dollar} vert JKMrangle {dollar}旋转状态。初始反应物量子态的选择与光产物的状态选择性检测相结​​合,可以确定化学反应可能的最大信息量。反过来,这可以确定分子特异性的跃迁偶极子矩阵元素(T-矩阵),其中包含化学反应的所有动力学信息。在第一个实验中,一束植入氙气中的氘化甲基碘光束{dollar} rm CDsb3I {dollar}(5-10%)被静电六极杆聚焦成{振动} vert 111rangle {dollar}无振动的旋转状态。然后,通过266 nm的激光在A带中将状态选择的分子光解离。然后,通过(2 + 1)REMPI,通过(2 + 1)REMPI测量甲基光碎片的几个单独旋转状态(低总角动量,{Jle 2){美元})的总体和排列(第二和第四级球面矩)。 {dollar} rm 3psp2Asbsp {lcub} 2 {rcub} {lcub} primeprime {rcub}得到2psp2Asbsp {lcub} 2 {rcub} {lcub} primeprime {rcub} {dollar}电子过渡。甲基光碎片的量子态特定角度分布是通过飞行时间(TOF)光谱法测量的。另外,从这些详细横截面的测量(积分和微分),计算出了T矩阵的元素,代表了光离解反应可能的最高细节水平。在第二个实验中,通过静电六极杆选择了用氩气(10-50%)填充亚硝酰氯(NOCl)束的状态,然后在{dollar} {lcub} sim {rcub} 355 {dollar}的B波段进行光解离纳米确定了几种产品一氧化氮(NO)旋转状态(高总角动量,{J} 39.5){美元}的角度分布,状态总体和旋转取向。产品NO旋转分布非常热,分布的峰值远高于{dollar} J = 30 {dollar},并且倾向于{dollar} {lcub} bf J {rcub} {dollar}(总角动量)垂直于实验室Z轴定向。从角度积分对准力矩和光碎裂角分布的测量,估计可能的T矩阵幅度和相位。

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