Abstract

We study the crystal-momentum-resolved contributions to the high-order harmonic generation (HHG) in band-gap materials, and identify the relevant initial crystal momenta for the first and higher plateaus of the HHG spectra. We do so by using a time-dependent density-functional theory model of one-dimensional linear chains. We introduce a self-consistent periodic treatment for the infinitely extended limit of the linear chain model, which provides a convenient way to simulate and discuss the HHG from a perfect crystal beyond the single-active-electron approximation. The multi-plateau spectral feature is elucidated by a semiclassical k-space trajectory analysis with multiple conduction bands taken into account. In the considered laser-interaction regime, the multiple plateaus beyond the first cutoff are found to stem mainly from electrons with initial crystal momenta away from the Gamma point (k = 0), while electrons with initial crystal momenta located around the Gamma point are responsible for the harmonics in the first plateau. We also show that similar findings can be obtained from calculations using a sufficiently large finite model, which proves to mimic the corresponding infinite periodic limit in terms of the band structures and the HHG spectra.

Highlights

  • High-order harmonic generation (HHG) in solids has attracted great attention since its experimental observation in 2011 [1], and its underlying mechanism is still being debated [2,3,4,5,6,7,8,9,10,11,12]

  • For typical laser parameters considered so far, it has been demonstrated that the orbitals in the highest-occupied band VB2 dominantly contribute to the total high-order harmonic generation (HHG) spectra [49]

  • We numerically studied the HHG from a model solid with a band gap irradiated by linearly polarized laser pulses, in particular the multiplateau spectral structures

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Summary

INTRODUCTION

High-order harmonic generation (HHG) in solids has attracted great attention since its experimental observation in 2011 [1], and its underlying mechanism is still being debated [2,3,4,5,6,7,8,9,10,11,12]. Capturing the idea of the simple-man model for atomic HHG [24], a generalized three-step model [11,21] was proposed for the interband HHG in solids It involves the following steps: (i) Near the peak of the laser field, an electron tunnels from the valence band to the conduction band, producing a hole in the valence band; (ii) the electron and hole move in the corresponding bands, driven by the external field; and (iii) they recombine and emit HHG radiation with a frequency corresponding to the band energy difference at the crystal momentum at which the recombination occurs. Atomic units (a.u.) are used throughout unless stated otherwise

Finite chain model
Infinitely extended chain model
Finite versus periodic
Multiple plateaus from a many-electron reciprocal-space perspective
Contribution of different orbitals to HHG
CONCLUSION
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