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Simultaneous phase control of Li_2 wave packets in two electronic states

机译:两种电子状态下Li_2波包的同时相位控制

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State-selective phase control of rotational Li_2 wave packets, prepared simultaneously in the E(~1#SIGMA#_g~+) electronic state by one photon absorption and the A(~1#SIGMA#_u~+) electronic state by resonant impulsive stimulated Raman scattering, is demonstrated. Following the initial population of a rovibrational launch state on the A electronic potential energy curve with a cw laser, a single sub-picosecond wave packet preparation pulse centered near 800 nm simultaneously creates a two-state rotational wave packet in the E state (v_E=18, J_E=23 and 25) and a three-state rotational wave packet in the A state (v_A=15, J_A=22,24, and 26). A temporally delayed 800 nm probe pulse subsequently ionizes both electronic components of the wave packet to allow measurement of the time-dependent coherence in these two electronic states. Via phase manipulation of resonant transition frequencies contained within the preparation pulse, the phases of the E(18,25) and A(15,26) quantum states are either varied concurrently or individually controlled, whereas the phases of the other rovibronic states of the wave packet are in all cases held essentially constnat. This phase manipulation is shown to be more complex than a simple additive effect involving the phases applied to the resonant frequencies. These experimental results are compared with the prredictions of second order time-dependent perturbation theory. Although systematic discrepancies exist, most likely due to an additional phase introduced during the two-photon probe process, once these differences are accounted for, good agreement is found between experiment and perturbation theory.
机译:旋转Li_2波包的状态选择相位控制,通过一个光子吸收同时在E(〜1#SIGMA#_g〜+)电子状态和共振脉冲在A(〜1#SIGMA#_u〜+)电子状态下同时准备证明了受激拉曼散射。跟随连续激光在A电子势能曲线上的旋转振动发射状态的初始填充之后,以近800 nm为中心的单个亚皮秒波包准备脉冲同时在E状态下创建了一个两态旋转波包(v_E = 18,J_E = 23和25)和处于A状态的三态旋转波包(v_A = 15,J_A = 22,24和26)。随时间延迟的800 nm探测脉冲随后将波包的两个电子成分电离,从而可以测量这两个电子状态下随时间变化的相干性。通过对预备脉冲中包含的共振跃迁频率进行相位控制,可以同时或单独控制E(18,25)和A(15,26)量子态的相位,而该量子态的其他旋转电子态的相位在所有情况下,波包基本上都保持恒定。事实表明,这种相位控制比简单的累加效应(涉及施加到谐振频率的相位)要复杂得多。将这些实验结果与二阶时间相关摄动理论的理论进行了比较。尽管存在系统上的差异,但很可能是由于在双光子探测过程中引入了一个附加相,所以一旦解决了这些差异,就可以在实验和微扰理论之间找到很好的一致性。

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