Ionization-assisted guided-wave pulse compression to extreme peak powers and single-cycle pulse widths in the mid-infrared

2010 ◽  
Vol 35 (21) ◽  
pp. 3640 ◽  
Author(s):  
A. A. Voronin ◽  
V. M. Gordienko ◽  
V. T. Platonenko ◽  
V. Ya. Panchenko ◽  
A. M. Zheltikov
Author(s):  
Tobias Witting ◽  
William A. Okell ◽  
Davide Fabris ◽  
Dane Austin ◽  
Maimouna Bacoum ◽  
...  

Author(s):  
Peter Krogen ◽  
Houkun Liang ◽  
Kevin Zawilski ◽  
Peter Schunemann ◽  
Kyung-Han Hong ◽  
...  

Author(s):  
Bruno E. Schmidt ◽  
Pierre Béjot ◽  
Andrew D. Shiner ◽  
Philippe Lassonde ◽  
Carlos Trallero-Herrero ◽  
...  

CLEO: 2014 ◽  
2014 ◽  
Author(s):  
Ayhan Demircan ◽  
Shalva Amiranashvili ◽  
Carsten Bree ◽  
Uwe Morgner ◽  
Gunter Steinmeyer

2020 ◽  
Vol 28 (7) ◽  
pp. 9099 ◽  
Author(s):  
F. Köttig ◽  
D. Schade ◽  
J. R. Koehler ◽  
P. St. J. Russell ◽  
F. Tani

2021 ◽  
Author(s):  
Rostislav Arkhipov ◽  
Mikhail Arkhipov ◽  
Ayhan Demircan ◽  
Uwe Morgner ◽  
Ihar Babushkin ◽  
...  

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.


Nanophotonics ◽  
2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Ali Rostamian ◽  
Ehsan Madadi-Kandjani ◽  
Hamed Dalir ◽  
Volker J. Sorger ◽  
Ray T. Chen

Abstract Thanks to the unique molecular fingerprints in the mid-infrared spectral region, absorption spectroscopy in this regime has attracted widespread attention in recent years. Contrary to commercially available infrared spectrometers, which are limited by being bulky and cost-intensive, laboratory-on-chip infrared spectrometers can offer sensor advancements including raw sensing performance in addition to use such as enhanced portability. Several platforms have been proposed in the past for on-chip ethanol detection. However, selective sensing with high sensitivity at room temperature has remained a challenge. Here, we experimentally demonstrate an on-chip ethyl alcohol sensor based on a holey photonic crystal waveguide on silicon on insulator-based photonics sensing platform offering an enhanced photoabsorption thus improving sensitivity. This is achieved by designing and engineering an optical slow-light mode with a high group-index of n g  = 73 and a strong localization of modal power in analyte, enabled by the photonic crystal waveguide structure. This approach includes a codesign paradigm that uniquely features an increased effective path length traversed by the guided wave through the to-be-sensed gas analyte. This PIC-based lab-on-chip sensor is exemplary, spectrally designed to operate at the center wavelength of 3.4 μm to match the peak absorbance for ethanol. However, the slow-light enhancement concept is universal offering to cover a wide design-window and spectral ranges towards sensing a plurality of gas species. Using the holey photonic crystal waveguide, we demonstrate the capability of achieving parts per billion levels of gas detection precision. High sensitivity combined with tailorable spectral range along with a compact form-factor enables a new class of portable photonic sensor platforms when combined with integrated with quantum cascade laser and detectors.


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