Abstract
So far, it has been assumed that selective excitation of a desired valley in the Brillouin zone of a hexagonal two-dimensional material has to rely on using circularly polarized fields. We theoretically demonstrate a way to control the valley excitation in hexagonal 2D materials on a few-femtosecond timescale using a few-cycle, linearly polarized pulse with controlled carrier–envelope phase. The valley polarization is mapped onto the strength of the perpendicular harmonic signal of a weak, linearly polarized pulse, which allows to read this information all-optically without destroying the valley state and without relying on the Berry curvature, making our approach potentially applicable to inversion-symmetric materials. We show applicability of this method to hexagonal boron nitride and M o S 2 .
Highlights
Generation of few-cycle laser pulses with controlled electric field oscillations under the envelope, i.e. controlled carrier envelope phase (CEP), catalyzed the development of attosecond physics and technology, providing tools to control electron dynamics on sub-laser-cycle time scale [1, 2]
Attosecond technology has started to develop its potential in condensed matter, in particular via high harmonic generation (HHG) [3,4,5,6,7,8,9]
The practical possibility of shaping individual oscillations of an optical laser pulse marks first steps towards lightwave electronics – the sub-cycle monitoring and steering of electronic dynamics [10, 11] in solids, which holds the potential to increase the speed of information processing from the current GHz to the PHz rate (PHz lightwave electronics.)
Summary
Generation of few-cycle laser pulses with controlled electric field oscillations under the envelope, i.e. controlled carrier envelope phase (CEP), catalyzed the development of attosecond physics and technology, providing tools to control electron dynamics on sub-laser-cycle time scale [1, 2]. High circularity of the harmonic emission offers a method to generate highly elliptic attosecond pulses with a linearly polarized driver, in an all-solid-state setup. When CEP=0○, the electric field has a single dominant peak and the vector potential is zero at this peak, which leads to no valley polarization.
Published Version (Free)
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have