Abstract

The quantum phases of the electron paths driven by an ultrafast laser in high harmonic generation in an atomic gas depends linearly on the instantaneous cycle-averaged laser intensity. Using high laser intensities, a complete single ionisation of the atomic gas may occur before the laser pulse peak. Therefore, high harmonic generation could be localised only in a temporal window at the leading edge of laser pulse envelope. Varying the laser frequency chirp of an intense ultrafast laser pulse, the centre, and the width of the temporal window, that the high harmonic generation phenomenon occurs, could be controlled with high accuracy. This way, both the duration and the phase of the electron trajectories, that generate efficiently high harmonics, is fully controlled. A method of spectral control and selection of the high harmonic extreme ultraviolet light from distinct quantum paths is experimentally demonstrated. Furthermore, a phenomenological numerical model enlightens the physical processes that take place. This novel approach of the electron quantum path selection via laser chirp is a simple and versatile way of controlling the time-spectral characteristics of the coherent extreme ultraviolet light with applications in the fields of attosecond pulses and soft x-ray nano-imaging.

Highlights

  • The quantum phases of the electron paths driven by an ultrafast laser in high harmonic generation in an atomic gas depends linearly on the instantaneous cycle-averaged laser intensity

  • We have performed a systematic investigation of high harmonic generation (HHG) in argon gas semi-infinite cell measuring the high harmonic spectrum as a function of the generating laser pulse chirp

  • Our experimental results and theoretical treatment clearly show that the frequency chirp of the ultrafast laser pulses is a crucial parameter for the control of the electron quantum paths in the HHG from atomic gases

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Summary

Introduction

The quantum phases of the electron paths driven by an ultrafast laser in high harmonic generation in an atomic gas depends linearly on the instantaneous cycle-averaged laser intensity. A phenomenological numerical model enlightens the physical processes that take place This novel approach of the electron quantum path selection via laser chirp is a simple and versatile way of controlling the time-spectral characteristics of the coherent extreme ultraviolet light with applications in the fields of attosecond pulses and soft x-ray nano-imaging. Laser pulse peak intensities of the orders of 1013−1016 W/cm[2] are routinely available in laboratories worldwide The interaction of such strong laser pulses with atoms unveiled new strong field phenomena such as above threshold i­onisation[2,3], tunnelling ­ionisation[4], over the barrier i­onisation[5,6], as well as high harmonic generation (HHG)[7] allowing for coherent spectral sources in the XUV region.

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