Abstract

We present a semi-classical study of the effects of the Lorentz force on electrons during high harmonic generation in the soft and hard X-ray regions driven by near- and mid-infrared lasers with wavelengths from 0.8 to 20 μm, and at intensities below 1015 W/cm2. The transverse extent of the longitudinal Lorentz drift is compared for both Gaussian focus and waveguide geometries. Both geometries exhibit a longitudinal electric field component that cancels the magnetic Lorentz drift in some regions of the focus, once each full optical cycle. We show that the Lorentz force contributes a super-Gaussian scaling which acts in addition to the dominant high harmonic flux scaling of λ-(5-6) due to quantum diffusion. We predict that the high harmonic yield will be reduced for driving wavelengths > 6 μm, and that the presence of dynamic spatial mode asymmetries results in the generation of both even and odd harmonic orders. Remarkably, we show that under realistic conditions, the recollision process can be controlled and does not shut off completely even for wavelengths >10 μm and recollision energies greater than 15 keV.

Highlights

  • High harmonic generation (HHG) is an extreme nonlinear response of atoms to intense femtosecond laser fields, which makes it possible to upconvert ultraviolet, visible, and infrared (IR) laser light to much higher photon energies

  • We present a semi-classical study of the influence of the Lorentz force on electron trajectories during high harmonic generation driven by near- and mid-infrared lasers with wavelengths from 0.8 to 20 μm, and at optimal intensities up to 1015 W/cm2

  • We find that the longitudinal electric field at the focus can readily cancel the magnetic Lorentz drift

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Summary

Introduction

High harmonic generation (HHG) is an extreme nonlinear response of atoms to intense femtosecond laser fields, which makes it possible to upconvert ultraviolet, visible, and infrared (IR) laser light to much higher photon energies. We investigate the longitudinal deflection induced by the Lorentz v × B force combined with the longitudinal component of the electric field of a confined laser focus, to show how the overall displacement depends on the driving laser wavelength, intensity, mode size, and HHG geometry. We investigate the geometry most successful for soft X-ray HHG to date, a gas-filled hollow waveguide, and compare it with a free-focus gas cell/jet geometry. In both cases, we find that the longitudinal electric field at the focus can readily cancel the magnetic Lorentz drift.

Lorentz drift derivation
Recombination probability PR
Scaling of the recombination probability ratio with laser wavelength
X-ray spatial profiles in Gaussian foci and in waveguides
Conclusions
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