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Attosecond Ionization And Tunneling Delay Time Measurements In Helium

机译:氦中的阿秒电离和隧穿延迟时间测量

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It is well established that electrons can escape from atoms through tunneling under the influence of strong laser fields, but the timing of the process has been controversial and far too rapid to probe in detail. We used attosecond angular streaking to place an upper limit of 34 attoseconds and an intensity-averaged upper limit of 12 attoseconds on the tunneling delay time in strong field ionization of a helium atom. The ionization field derives from 5.5-femtosecond-long near-infrared laser pulses with peak intensities ranging from 2.3 × 10~(14) to 3.5 × 10~(14) watts per square centimeter (corresponding to a Keldysh parameter variation from 1.45 to 1.17, associated with the onset of efficient tunneling). The technique relies on establishing an absolute reference point in the laboratory frame by elliptical polarization of the laser pulse, from which field-induced momentum shifts of the emergent electron can be assigned to a temporal delay on the basis of the known oscillation of the field vector.
机译:众所周知,电子可以在强激光场的影响下通过隧穿从原子中逸出,但是该过程的时间安排一直存在争议,而且太快了,无法进行详细探测。在氦原子强场电离过程中,我们使用了阿秒角条纹,将隧穿延迟时间的上限设为34阿秒,强度平均上限设为12阿秒。电离场源自5.5飞秒长的近红外激光脉冲,其峰值强度范围为每平方厘米2.3×10〜(14)到3.5×10〜(14)瓦(对应于Keldysh参数从1.45到1.17的变化) ,与有效隧穿的开始有关)。该技术依赖于通过激光脉冲的椭圆极化在实验室框架中建立绝对参考点,基于已知的场矢量振荡,可以将新兴电子的场致动量位移分配给时间延迟。 。

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