Generation and multi-octave shaping of mid-infrared intense single-cycle pulses

2017 ◽  
Vol 11 (4) ◽  
pp. 222-226 ◽  
Author(s):  
Peter Krogen ◽  
Haim Suchowski ◽  
Houkun Liang ◽  
Noah Flemens ◽  
Kyung-Han Hong ◽  
...  
Keyword(s):  
Author(s):  
Peter Krogen ◽  
Houkun Liang ◽  
Kevin Zawilski ◽  
Peter Schunemann ◽  
Kyung-Han Hong ◽  
...  

2015 ◽  
Vol 40 (3) ◽  
pp. 423 ◽  
Author(s):  
Yutaka Nomura ◽  
Yu-Ting Wang ◽  
Atsushi Yabushita ◽  
Chih-Wei Luo ◽  
Takao Fuji

2020 ◽  
Vol 9 (1) ◽  
Author(s):  
Xing-Long Zhu ◽  
Su-Ming Weng ◽  
Min Chen ◽  
Zheng-Ming Sheng ◽  
Jie Zhang

2019 ◽  
Vol 205 ◽  
pp. 05011
Author(s):  
Christoph P. Schmid ◽  
Fabian Langer ◽  
Stefan Schlauderer ◽  
Martin Gmitra ◽  
Jaroslav Fabian ◽  
...  

As conventional electronic is approaching its ultimate limits, tremendous efforts have been taken to explore novel concepts of ultrafast quantum control. Lightwave electronics - the foundation of attosecond science - has opened a spectacular perspective by utilizing the oscillating carrier wave of an intense light pulse to control the translational motion of the electron’s charge faster than a single cycle of light [1-7]. Despite their promising potential as future information carriers [8,10], the internal quantum attributes such as spins and valley pseudospins have not been switchable at optical clock rates. Here we demonstrate a novel subcycle control scheme of the electron’s pseudospin in a monolayer of tungsten diselenide using strong mid-infrared lightwaves [9]. Our work opens the door towards systematic valleytronic protocols at optical clock rates.


Author(s):  
Thomas Butler ◽  
Daniel Gerz ◽  
Christina Hofer ◽  
Jia Xu ◽  
Christian Gaida ◽  
...  
Keyword(s):  

Author(s):  
Takao Fuji ◽  
Yutaka Nomura ◽  
Hideto Shirai ◽  
Noriaki Tsurumachi ◽  
Alexander A. Voronin ◽  
...  
Keyword(s):  

2020 ◽  
Vol 45 (6) ◽  
pp. 1511 ◽  
Author(s):  
Sergey Chekalin ◽  
Alexander Dormidonov ◽  
Valerii Kandidov ◽  
Victor Kompanets

2018 ◽  
Vol 8 (12) ◽  
pp. 2451 ◽  
Author(s):  
Yuxi Fu ◽  
Hua Yuan ◽  
Katsumi Midorikawa ◽  
Pengfei Lan ◽  
Eiji Takahashi

We discuss the efficient generation of intense “water window” (0.28–0.54 keV) isolated attosecond pulses (IAPs) using a mid-infrared (MIR) waveform synthesizer. Our numerical simulations clearly indicate that not only a longer-wavelength driving laser but also a weak control pulse in the waveform synthesizer helps extend the continuum cutoff region and reduce the temporal chirp of IAPs in high-order harmonic generation (HHG). This insight indicates that a single-cycle laser field is not an optimum waveform for generating the shortest IAP from the veiwpoints of reducing the attochirp and increasing the efficiency of HHG. By combining a waveform synthesizer technology and a 100 mJ MIR femtosecond pulse based on a dual-chirped optical parametric amplification (DC-OPA) method, a gigawatt-scale IAP (55 as with 10 nJ order) in the water window region can be generated even without attochirp compensation. The MIR waveform synthesizer is highly beneficial for generating a shorter IAP duration in the soft X-ray region because there are no suitable transparent dispersive materials that can be used for compressing the attochirp.


Photonics ◽  
2021 ◽  
Vol 8 (8) ◽  
pp. 290
Author(s):  
Kan Tian ◽  
Linzhen He ◽  
Xuemei Yang ◽  
Houkun Liang

In the past decade, mid-infrared (MIR) few-cycle lasers have attracted remarkable research efforts for their applications in strong-field physics, MIR spectroscopy, and bio-medical research. Here we present a review of MIR few-cycle pulse generation and amplification in the wavelength range spanning from 2 to ~20 μm. In the first section, a brief introduction on the importance of MIR ultrafast lasers and the corresponding methods of MIR few-cycle pulse generation is provided. In the second section, different nonlinear crystals including emerging non-oxide crystals, such as CdSiP2, ZnGeP2, GaSe, LiGaS2, and BaGa4Se7, as well as new periodically poled crystals such as OP-GaAs and OP-GaP are reviewed. Subsequently, in the third section, the various techniques for MIR few-cycle pulse generation and amplification including optical parametric amplification, optical parametric chirped-pulse amplification, and intra-pulse difference-frequency generation with all sorts of designs, pumped by miscellaneous lasers, and with various MIR output specifications in terms of pulse energy, average power, and pulse width are reviewed. In addition, high-energy MIR single-cycle pulses are ideal tools for isolated attosecond pulse generation, electron dynamic investigation, and tunneling ionization harness. Thus, in the fourth section, examples of state-of-the-art work in the field of MIR single-cycle pulse generation are reviewed and discussed. In the last section, prospects for MIR few-cycle lasers in strong-field physics, high-fidelity molecule detection, and cold tissue ablation applications are provided.


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