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Abstract
Under strong laser fields, electrons in solids radiate high-harmonic fields by travelling through quantum pathways in Bloch bands in the sub-laser-cycle timescales. Understanding these pathways in the momentum space through the high-harmonic radiation can enable an all-optical ultrafast probe to observe coherent lightwave-driven processes and measure electronic structures as recently demonstrated for semiconductors. However, such demonstration has been largely limited for semimetals because the absence of the bandgap hinders an experimental characterization of the exact pathways. In this study, by combining electrostatic control of chemical potentials with HHG measurement, we resolve quantum pathways of massless Dirac fermions in graphene under strong laser fields. Electrical modulation of HHG reveals quantum interference between the multi-photon interband excitation channels. As the light-matter interaction deviates beyond the perturbative regime, elliptically polarized laser fields efficiently drive massless Dirac fermions via an intricate coupling between the interband and intraband transitions, which is corroborated by our theoretical calculations. Our findings pave the way for strong-laser-field tomography of Dirac electrons in various quantum semimetals and their ultrafast electronics with a gate control.
Under strong laser fields, materials exhibit extreme non-linear optical response, such as high harmonic generation. These higher harmonics provide insights into electron behaviour in materials in sub-laser cycle timescale. Here, Cha et al study higher harmonic generation resulting from the laser driven motion of massless Dirac fermions in graphene.
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1 Institute for Basic Science (IBS), Center for Van der Waals Quantum Solids, Pohang, Republic of Korea (GRID:grid.410720.0) (ISNI:0000 0004 1784 4496)
2 Institute for Basic Science (IBS), Center for Van der Waals Quantum Solids, Pohang, Republic of Korea (GRID:grid.410720.0) (ISNI:0000 0004 1784 4496); Pohang University of Science and Technology, Department of Materials Science and Engineering, Pohang, Republic of Korea (GRID:grid.49100.3c) (ISNI:0000 0001 0742 4007)
3 Daegu Gyeongbuk Institute of Science and Technology (DGIST), Department of Physics and Chemistry, Daegu, Republic of Korea (GRID:grid.417736.0) (ISNI:0000 0004 0438 6721)
4 Institute for Basic Science (IBS), Center for Van der Waals Quantum Solids, Pohang, Republic of Korea (GRID:grid.410720.0) (ISNI:0000 0004 1784 4496); Pohang University of Science and Technology, Department of Chemical Engineering, Pohang, Republic of Korea (GRID:grid.49100.3c) (ISNI:0000 0001 0742 4007)
5 Pohang University of Science and Technology, Department of Chemistry, Pohang, Republic of Korea (GRID:grid.49100.3c) (ISNI:0000 0001 0742 4007)
6 Institute for Basic Science (IBS), Center for Artificial Low Dimensional Electronic Systems, Pohang, Republic of Korea (GRID:grid.410720.0) (ISNI:0000 0004 1784 4496); Pohang University of Science and Technology, Department of Physics, Pohang, Republic of Korea (GRID:grid.49100.3c) (ISNI:0000 0001 0742 4007)
7 Institute for Basic Science (IBS), Center for Artificial Low Dimensional Electronic Systems, Pohang, Republic of Korea (GRID:grid.410720.0) (ISNI:0000 0004 1784 4496); Pohang University of Science and Technology, Department of Physics, Pohang, Republic of Korea (GRID:grid.49100.3c) (ISNI:0000 0001 0742 4007); Asia Pacific Center for Theoretical Physics, Pohang, Republic of Korea (GRID:grid.482264.e) (ISNI:0000 0000 8644 9730)
8 Institute for Basic Science (IBS), Center for Van der Waals Quantum Solids, Pohang, Republic of Korea (GRID:grid.410720.0) (ISNI:0000 0004 1784 4496); Pohang University of Science and Technology, Department of Materials Science and Engineering, Pohang, Republic of Korea (GRID:grid.49100.3c) (ISNI:0000 0001 0742 4007); Pohang University of Science and Technology, Department of Physics, Pohang, Republic of Korea (GRID:grid.49100.3c) (ISNI:0000 0001 0742 4007)