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首页> 外文期刊>The Journal of Chemical Physics >Photodynamics in superfluid helium: Femtosecond laser-induced ionization, charge recombination, and preparation of molecular Rydberg states
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Photodynamics in superfluid helium: Femtosecond laser-induced ionization, charge recombination, and preparation of molecular Rydberg states

机译:超流氦中的光动力学:飞秒激光诱导的电离,电荷重组和分子里德堡态的制备

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Femtosecond pulses (790 nm) are used for nonresonant laser excitation of superfluid liquid helium to prepare ionic and neutral excited states at energies above 18 eV. Measurements of laser-induced fluorescence and photocurrent enable a detailed description of the primary photoprocesses. A controllable excitation regime unique to femtosecond pulses is realized at laser intensities below the dielectric breakdown threshold, I < 5 * 10~(13) W/cm~2. A steady state of the long-lived triplet excimers He_(2~*)(~3a) (lowest Rydberg state) is established; the concentration decays between laser pulses through diffusion-controlled bimolecular annihilation to approx 10~(12) cm~(-3) at a laser repetition rate of 500 Hz. The triplet population is amplified with each pulse in a sequence that involves: (1) ionization of the Rydberg electron of He_(2~*) via complete Coulomb barrier suppression; (2) cascade electron impact ionization of the ground-state He atoms by the ponderomotively accelerated quasifree electrons in liquid He; (3) localization and thermalization of the "hot" electrons and He~+ cations to form electron "bubble" and He_(3~+) "snowball" states; (4) recombination of these elementary charge carriers to form He_(2~*). The amplification factor for the triplets M = 2~m characterizes the excitation sequence: m is the number of generations in the cascade (m = 5 at I = 4.5 * 10~(13) W/cm~2), and m is proportional to the laser intensity and temporal pulse width. The laser-induced ionization cascade prepares an inhomogeneous initial distribution of spatially separated ions on three length scales: clumps of positive charges with an interionic separation determined by the cascade length of 60 A; a cloud of electrons surrounding the clump at the electron thermalization length approx 10~3 A; and interclump separation dictated by the concentration of the He_(2~*) precursors, approx 10~4 A.
机译:飞秒脉冲(790 nm)用于超流体氦的非共振激光激发,以在18 eV以上的能量下制备离子和中性激发态。激光诱导的荧光和光电流的测量可以对主要的光过程进行详细描述。飞秒脉冲独有的可控激发机制是在低于介电击穿阈值I <5 * 10〜(13)W / cm〜2的激光强度下实现的。建立了长寿命三重态准分子He_(2〜*)(〜3a)的稳态(最低里德堡态);在500 Hz的激光重复频率下,通过扩散控制的双分子an灭,激光脉冲之间的浓度衰减到大约10〜(12)cm〜(-3)。通过每个脉冲以以下顺序放大三重态种群,该顺序包括:(1)通过完全库仑势垒抑制使He_(2〜*)的Rydberg电子电离; (2)通过液态He中的质子加速准自由电子对基态He原子进行级联电子碰撞电离; (3)“热”电子和He〜+阳离子的局部化和热化,形成电子“气泡”和He_(3〜+)“雪球”态; (4)将这些基本电荷载流子复合以形成He_(2〜*)。三元组的放大因子M = 2〜m表征了激发序列:m是级联中的世代数(在I = 4.5 * 10〜(13)W / cm〜2时m = 5),并且m与比例成正比激光强度和时间脉冲宽度。激光诱导的电离级联反应会在三个长度尺度上制备空间上分离的离子的不均匀初始分布:正离子团簇,其离子间距由60 A级联长度确定;在电子热化长度约10〜3 A时,簇状电子围绕云团;和簇间分离取决于He_(2〜*)前体的浓度,大约10〜4A。

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