Abstract

We have unveiled coherent multiphoton interferences originating from different quantum paths taken by the Auger electron induced by a high-intensity x-ray/extreme ultraviolet pulse under the presence of a strong optical field. These interferences give rise to a clear signature in the angle-resolved Auger electron spectrum: an asymmetry with respect to the energy of the Auger decay channel. In order to illustrate this effect we have considered the resonant Auger decay of the transition in Ne+. The simulations show that these interferences are very sensitive to the parameters of the x-ray and optical fields.

Highlights

  • Free-electron lasers (FELs) can achieve very high intensities, an important feature to produce nonlinear processes in the x-ray/XUV regime [1]

  • The sidebands are related to the above-threshold ionization (ATI) phenomenon [30], and analogously to ATI, every sideband-peak is separated by an optical photon energy

  • The main goal of this work is to unveil the origin and the main effects of the coherent multiphoton interferences described in the last section, we would like to provide a discussion of some factors that may play an important role for the observation of the asymmetries in the Auger electron spectrum

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Summary

INTRODUCTION

Free-electron lasers (FELs) can achieve very high intensities (more than 1015 W/cm2), an important feature to produce nonlinear processes in the x-ray/XUV regime [1]. The combination of x-ray/XUV light with strong optical fields (1010-1015W/cm2) introduces a new degree of controllability exceptionally beneficial for pump-probe experiments [17,18,19], optical control of x-ray absorption [20, 21], and x-ray pulse characterization [22]. In these experiments inner-shell holes are created and the Auger decay that follows provides an ultrafast internal probe of the electron dynamics. Our simulations show that these interferences are very sensitive to the x-ray and optical parameters due to the intrinsic coherence of the whole process

THEORETICAL MODEL
ORIGIN OF THE MULTIPHOTON INTERFERENCES
OBSERVATION OF THE ASYMMETRIES
CONCLUSIONS
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