Paulus G G, Grasbon F, Walther H, Villoresi P, Nisoli M, Stagira S, Priori E, De Silvestri S
Max-Planck-Institut für Quantenoptik, Hans-Kopfermann-Strasse 1, 85748 Garching bei München, Germany.
Nature. 2001 Nov 8;414(6860):182-4. doi: 10.1038/35102520.
Currently, the shortest laser pulses that can be generated in the visible spectrum consist of fewer than two optical cycles (measured at the full-width at half-maximum of the pulse's envelope). The time variation of the electric field in such a pulse depends on the phase of the carrier frequency with respect to the envelope-the absolute phase. Because intense laser-matter interactions generally depend on the electric field of the pulse, the absolute phase is important for a number of nonlinear processes. But clear evidence of absolute-phase effects has yet to be detected experimentally, largely because of the difficulty of stabilizing the absolute phase in powerful laser pulses. Here we use a technique that does not require phase stabilization to demonstrate experimentally the influence of the absolute phase of a short laser pulse on the emission of photoelectrons. Atoms are ionized by a short laser pulse, and the photoelectrons are recorded with two opposing detectors in a plane perpendicular to the laser beam. We detect an anticorrelation in the shot-to-shot analysis of the electron yield.
目前,在可见光谱中能够产生的最短激光脉冲包含不到两个光学周期(在脉冲包络的半高全宽处测量)。这种脉冲中电场的时间变化取决于载波频率相对于包络的相位——绝对相位。由于强激光与物质的相互作用通常取决于脉冲的电场,因此绝对相位对于许多非线性过程都很重要。但是,绝对相位效应的明确证据尚未通过实验检测到,这主要是因为在强激光脉冲中稳定绝对相位存在困难。在这里,我们使用一种不需要相位稳定的技术,通过实验证明短激光脉冲的绝对相位对光电子发射的影响。原子被短激光脉冲电离,光电子由两个相对的探测器在垂直于激光束的平面上记录。我们在电子产额的逐次分析中检测到了反相关性。