Source abstract
Abstract
Various interference effects are known to exist in the process of high harmonic generation (HHG) both at the single atom and macroscopic levels (Kanai, T.; et al. Nature 2005, 435, 470–474; Zaı̈r, A.; et al. Phys. Rev. Lett. 2008, 100, 143902; Heyl, C. M.; et al. Phys. Rev. Lett. 2011, 107, 033903). In particular, the quantum path difference between the long and short trajectories of electron excursion causes the HHG yield to experience interference-based temporal and spectral modulations (He, L.; et al. Phys. Rev. A 2015, 92, 043403; Nefedova, V. E.; et al. Phys. Rev. A 2018, 98, 033414). In solids, due to additional phenomena such as multiband superposition (Hohenleutner, M.; et al. Nature 2015, 523, 572–575) and crystal symmetry dependency (Langer, F.; et al. Nat. Photonics 2017, 11, 227–231; Liu, H.; et al. Nat. Phys. 2017, 13, 262–265), the HHG mechanism appears to be more complicated than in gaseous atoms in identifying accompanying interference phenomena. Here, we first report experimental data showing intensity-dependent spectral modulation and broadening of high harmonics observed from bulk sapphire. Then, by adopting theoretical simulation, the extraordinary observation is interpreted as a result of the quantum path interference between the long and short electron/hole trajectories. Specifically, the long trajectory undergoes an intensity-dependent redshift, which coherently combines with the short trajectory to exhibit spectral splitting in an anomalous way of inverse proportion to the driving laser intensity. This quantum interference may be extended to higher harmonics with increasing the laser intensity, underpinning the potential for precise control of the phase matching and modulation, even in the extreme ultraviolet and soft X-ray regime. Further, this approach may act as a novel tool for probing arbitrary crystals so as to adjust the electron dynamics of higher harmonics for attosecond spectroscopy.
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Affiliations
Department of Mechanical Engineering, Korea Advanced Institute of Science and Technology (KAIST), 291 Daehak-ro, Yuseong-gu, Daejeon 34141, South Korea
State Key Laboratory of Magnetic Resonance and Atomic and Molecular Physics, Wuhan Institute of Physics and Mathematics, Chinese Academy of Sciences, Wuhan 430071, China
School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
Institute for the Frontier of Attosecond Science and Technology, CREOL and Department of Physics, University of Central Florida, Orlando, Florida 32816, United States
Department of Optics and Mechatronics Engineering, College of Nanoscience and Nanotechnology, Pusan National University, 2 Busandaehak-ro 63beon-gil, Busan 46241, South Korea
Institute of Physics of the ASCR, ELI-Beamlines Project, Na Slovance 2, 182 21 Prague, Czech Republic
Funding
National Natural Science Foundation of China · National Research Foundation of Korea