2021
DOI: 10.1364/oe.412639
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Transverse phase matching of high-order harmonic generation in single-layer graphene

Abstract: The efficiency of high-harmonic generation (HHG) from a macroscopic sample is strongly linked to the proper phase matching of the contributions from the microscopic emitters. We develop a combined micro+macroscopic theoretical model that allows us to distinguish the relevance of high-order harmonic phase matching in single-layer graphene. For a Gaussian driving beam, our simulations show that the relevant HHG emission is spatially constrained to a phase-matched ring around the beam axis. This remarkable findin… Show more

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Cited by 9 publications
(6 citation statements)
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References 63 publications
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“…HHG driven by structured beams requires the computation of the macroscopic response of the target. Our strategy follows the discrete-dipole approximation method presented in [54], that has been recently also applied to graphene polycrystals [55]. In this method, the graphene target is divided into a set of elemental surfaces of dimensions small enough to assume the local field profile constant, but still enclosing a sufficient number of graphene's lattice cells to allow the approximation of the Brillouin zone as a continuous region.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…HHG driven by structured beams requires the computation of the macroscopic response of the target. Our strategy follows the discrete-dipole approximation method presented in [54], that has been recently also applied to graphene polycrystals [55]. In this method, the graphene target is divided into a set of elemental surfaces of dimensions small enough to assume the local field profile constant, but still enclosing a sufficient number of graphene's lattice cells to allow the approximation of the Brillouin zone as a continuous region.…”
Section: Methodsmentioning
confidence: 99%
“…The dipole acceleration is used to compute the time derivative of the current density, which is proportional to the radiated near-field, and used as a source for the electromagnetic field propagator, in order to find the far-field distribution. Dynamics of the SLG interaction with the driving field is integrated from the Schrödinger equation in the nearest neighbor tight-binding approximation [12,54].…”
Section: Methodsmentioning
confidence: 99%
“…To compute HHG from SLG we follow [9]. First, we discretize the target layer into elemental surface elements, small enough to consider the driver's profile along them as constant.…”
Section: Harmonic Near-field Distributionmentioning
confidence: 99%
“…Particularly, HHG from solid targets has incited significant interest due to their higher density, which engenders a qualitative enhancement in harmonic conversion efficiency, a consequence of the coherent nature of the process [32][33][34][35][36]. Currently, there has been a burgeoning interest in understanding the nonlinear optical response of lower-dimensional materials, such as 2D graphene [37][38][39][40][41][42][43][44][45][46][47], silicene [48], MoS 2 [49], or hBN [50][51][52], and 1D silicon nanotubes [53] or CNTs [54][55][56]. For instance, the generation of up to the 9th harmonic in gapless graphene has been observed using a mid-infrared driving laser [57,58].…”
Section: Introductionmentioning
confidence: 99%