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首页> 外文期刊>Journal of physics, A. Mathematical and theoretical >Exact solution of the 1D time-dependent Schrodinger equation for the emission of quasi-free electrons from a flat metal surface by a laser
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Exact solution of the 1D time-dependent Schrodinger equation for the emission of quasi-free electrons from a flat metal surface by a laser

机译:1D时间依赖性Schrodinger方程的精确解决方案,用于通过激光从扁平金属表面发射无准电子

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We solve exactly the one-dimensional Schrodinger equation for psi(x,t) describing the emission of electrons from a flat metal surface, located atx= 0, by a periodic electric field E cos(omega t) at x> 0, turned on att= 0. We prove that for all physical initial conditions psi(x, 0), the solution psi(x,t) exists, and converges for long times, at a rate t(-3/2), to a periodic solution considered by Faisalet al(2005Phys. Rev.A72023412). Using the exact solution, we compute psi(x,t), for t> 0, via an exponentially convergent algorithm, taking as an initial condition a generalized eigenfunction representing a stationary state for E = 0. We find, among other things, that: (i) the time it takes the current to reach its asymptotic state may be large compared to the period of the laser; (ii) the current averaged over a period increases dramatically as h omega becomes larger than the work function of the metal plus the ponderomotive energy in the field. For weak fields, the latter is negligible, and the transition is at the same frequency as in the Einstein photoelectric effect; (iii) the current at the interface exhibits a complex oscillatory behavior, with the number of oscillations in one period increasing with the laser intensity and period. These oscillations get damped strongly as x increases.
机译:我们恰好地解决了PSI(X,T)的一维Schrodinger方程,所述PSI(x,t)描述从扁平金属表面,位于ATX = 0,通过X> 0处的周期性电场E COS(OMEGA T),打开ATT = 0.我们证明对于所有物理初始条件PSI(x,0),解决PSI(X,T)存在,并且长时间收敛于速率T(-3/2),以定期解决方案由Faisalet al(2005phys rev.a72023412)考虑。使用精确的解决方案,我们通过指数收敛算法计算PSI(x,t),用于t> 0,作为初始条件,作为e = 0表示静止状态的广义特征函数。除其他外,我们发现了:(i)与激光器相比,电流达到其渐近状态所需的时间; (ii)随着Homega大于金属的功率加上该领域的思考能量大幅增加,在一段时间内平均的电流急剧增加。对于弱领域,后者可以忽略不计,并且转换与爱因斯坦光电效应相同。 (iii)界面处的电流表现出复杂的振荡行为,在一个时期随着激光强度和时段增加一个时期的振荡数。随着x增加,这些振荡强烈抑制。

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