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首页> 外文期刊>Physical Review, A >Nonconstant ponderomotive energy in above-threshold ionization by intense short laser pulses
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Nonconstant ponderomotive energy in above-threshold ionization by intense short laser pulses

机译:通过强烈的短激光脉冲在上阈值电离中的不符合抗性电离能量

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We analyze the contribution of the quiver kinetic energy acquired by an electron in an oscillating electric field of a short laser pulse to the energy balance in atomic ionization processes. Due to the time dependence of this additional kinetic energy, a temporal average is assumed to preserve a stationary energy conservation rule, which is used to predict the position of the energy peaks observed in the photoelectron (PE) spectra. For a plane wave and a flattop pulse, the mean value of the quiver energy over the whole pulse leads to the concept of ponderomotive energy Up. However, for a short pulse with a fast changing intensity, the stationary approximation loses its validity. We check these concepts by studying first the PE spectrum within the semiclassical model (SCM) for multiple-step pulses. The SCM offers the possibility to establish a connection between emission times and the PE spectrum in the energy domain. We show that PE substructures stem from ionization at different times mapping the pulse envelope. We also analyze the PE spectrum for a realistic sine-squared envelope within the Coulomb-Volkov and ab initio calculations solving the time-dependent Schrodinger equation. We found that the electron emission amplitudes produced at different times interfere with each other producing, in this way, a new additional pattern that modulates the above-threshold ionization (ATI) peaks.
机译:我们分析了在短激光脉冲的振荡电场中通过电子获得的抖动动能的贡献,以原子电离过程中的能量平衡。由于这种额外的动能的时间依赖性,假设时间平均值保留静止节能规则,该规则用于预测在光电子(PE)光谱中观察到的能量峰的位置。对于平面波和扁平脉冲,整个脉冲上的颤动能量的平均值导致了追逐思考能量的概念。然而,对于具有快速变化强度的短脉冲,静止近似失去了其有效性。我们通过第一次在半半径模型(SCM)内的PE频谱来检查这些概念,用于多步脉冲。 SCM提供了在能量域中的发射时间和PE光谱之间建立连接的可能性。我们表明PE子结构源于不同时间绘制脉冲包络的电离。我们还分析了库仑-Volkov和AB Initio计算中的现实正弦平方体的PE谱,求解时间依赖的Schrodinger方程。我们发现在不同时间产生的电子发射幅度以这种方式互相干扰,以这种方式对其产生一种新的附加图案,其调节上述阈值电离(ATI)峰值。

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