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Interband resonant high-harmonic generation by valley polarized electron-hole pairs

TLDR
Even and odd high-harmonic generation up to 15th order from a variety of monolayers with different band properties are shown and the role of nonlinear interband polarization is emphasized.
Abstract
We demonstrated nonperturbative high harmonics induced by intense mid-infrared light up to 18th order that well exceed the material bandgap in monolayer transition metal dichalcogenides. The intensities of the even-order high-harmonic radiation did not monotonically decrease as the harmonic order increased. By comparing the high harmonic spectra with the optical absorption spectra, we found that the enhancement in the even-order high harmonics could be attributed to the resonance to the band nesting energy. The symmetry analysis shows that the valley polarization and anisotropic band structure lead to polarization of the high-harmonic radiation under excitation with the polarization along the zigzag direction. We also examined the possible recombination pathways of electrons and holes by calculating their dynamics in real and momentum spaces based on three-step model in solids. It revealed that, by considering the electrons and holes generated at neighboring lattice sites, the electron-hole polarization driven to the band nesting region should contribute to the high harmonic radiation. Our findings open the way for attosecond science with monolayer materials having widely tunable electronic structures.

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Strong-field nano-optics

TL;DR: In the strong-field regime, the amplitude and phase of the external electromagnetic field can exceed or exceed the field strengths that bind the electrons inside the medium as mentioned in this paper. But this is not the case in the non-perturbative regime.
Journal ArticleDOI

Chiral photocurrent in parity-violating magnet and enhanced response in topological antiferromagnet

TL;DR: In this article, a comprehensive classification of the photocurrent response arising from parity violation in bulk systems is presented, and a new type of photocurrent phenomena characteristic of parity-violating magnets, intrinsic Fermi surface effect and gyration current is found.
Journal ArticleDOI

High-harmonic generation in one-dimensional Mott insulators

TL;DR: In this article, the authors studied high-harmonic generation in the one-dimensional Hubbard model in order to understand its relation to elementary excitations as well as the similarities and differences to semiconductors.
References
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Journal ArticleDOI

Atomically thin MoS2: a new direct-gap semiconductor

TL;DR: The electronic properties of ultrathin crystals of molybdenum disulfide consisting of N=1,2,…,6 S-Mo-S monolayers have been investigated by optical spectroscopy and the effect of quantum confinement on the material's electronic structure is traced.
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Emerging Photoluminescence in Monolayer MoS2

TL;DR: This observation shows that quantum confinement in layered d-electron materials like MoS(2), a prototypical metal dichalcogenide, provides new opportunities for engineering the electronic structure of matter at the nanoscale.
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Coupled spin and valley physics in monolayers of MoS2 and other group-VI dichalcogenides.

TL;DR: It is shown that inversion symmetry breaking together with spin-orbit coupling leads to coupled spin and valley physics in monolayers of MoS2 and other group-VI dichalcogenides, making possible controls ofspin and valley in these 2D materials.
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Spin and pseudospins in layered transition metal dichalcogenides

TL;DR: In this article, the authors provide a brief review of both theoretical and experimental advances in this field and uncover the interplay between real spin and pseudospins in layered transition metal dichalcogenides.
Journal ArticleDOI

Exciton Binding Energy and Nonhydrogenic Rydberg Series in Monolayer WS 2

TL;DR: Strong but unconventional electron-hole interactions are expected to be ubiquitous in atomically thin materials using a microscopic theory in which the nonlocal nature of the effective dielectric screening modifies the functional form of the Coulomb interaction.
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