Showing posts with label laser induced air-plasma. Show all posts
Showing posts with label laser induced air-plasma. Show all posts

Tuesday, April 10, 2018

Abstract-Terahertz photonics of microplasma and beyond


X.C. ZHANG, F. BUCCHERI

http://www.lmaleidykla.lt/ojs/index.php/physics/article/view/3647

THz air photonics using laser-induced air plasma is one of the leading frontiers in the THz community. Ambient air, when excited with an intense femtosecond laser beam, exhibits the remarkable ability to generate and detect pulsed THz waves through a nonlinear optical process. Significant advances in the use of air plasma for emitting, controlling, enhancing and measuring broadband THz waves have opened up a range of research opportunities. However, one of the major challenges for the research community and in real world applications is that plasma formation requires the use of an intense laser (mJ pulse energy), but most femtosecond laser oscillators only have pulse energies in the range of pJ to tens of nJ. The investigation of THz photonics, specifically the exploration of laserinduced plasmas at the micro-nano scale and beyond, is a frontier. Microplasmas generated by tightly focused optical excitation beams with controlled polarization serve as a new THz source with its unique radiation pattern and easy operation. The laser energy threshold for THz wave generation, the power scaling and the generation efficiency from microplasmas are significantly different from those of elongated plasmas. Our estimation indicates that the micronano plasma approach could reduce the necessary optical pulse energy by five orders of magnitude, while still obtaining a comparable or better signal-to-noise ratio for THz time-domain spectroscopy. This would be made possible by the high electron density (1019 cm–3 or more) achievable with a tight focus laser excitation, which correlates with the THz generation efficiency, and the use of laser oscillators with a much higher pulse repetition rate, as compared to the currently employed amplified laser systems (100 MHz vs 1 kHz). The THz micro-nano plasma is expected to lead to key technologies that will enable further interdisciplinary research and continued advancements of numerous THz wave sensing and spectroscopy developments. It serves as a vehicle for studying the extreme THz science.

Friday, April 10, 2015

Abstract-Terahertz wave absorption via femtosecond laser-filament concatenation


http://opticalengineering.spiedigitallibrary.org/article.aspx?articleid=2272700
Ji Zhao, YueJin Zhao
Beijing Institute of Technology, School of Optoelectronics, Beijing Key Laboratory for Precision Optoelectronic Measurement Instrument and Technology, Room 6014, Optoelectronics Building, South Street of Zhongguancun, Beijing 100081, China
LiangLiang Zhang, Tong Wu, XiaoYan Xu, CunLin Zhang
Capital Normal University, Ministry of Education, Beijing Key Laboratory for Terahertz Spectroscopy and Imaging, Key Laboratory of Terahertz Optoelectronics, Beijing 100048, China
Opt. Eng. 54(4), 046104 (Apr 09, 2015). doi:10.1117/1.OE.54.4.046104

Abstract.  Terahertz (THz) emission from laser-induced air plasma is a well known and widely used phenomenon. We report that when two laser beams from the laser creating two plasma filaments interact with each other, THz absorption is observed. We believe that a change in the refractive index of the plasma causes the THz-wave absorption. The following experimental results reveal that the THz absorption becomes more pronounced with increasing pump power and that the gas species surrounding the femtosecond laser filament can also influence the THz absorption rate.
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Friday, July 25, 2014

Abstract-Frequency spectrum characterization of terahertz emission from laser-induced air plasma


Ji Zhao   Liangliang Zhang   Yiman Luo   Tong Wu   Cunlin Zhang   Yuejin Zhao 

http://www.opticsjournal.net/abstract.htm?id=OJ140723000036cIfLhO

Terahertz (THz) emission from laser-induced air-plasma is presented. The frequency spectra of THz wave are investigated using an air-biased-coherent-detection method. The frequency spectra are measured under different pump-pulse and probe-pulse energies. The frequency spectra become narrow with the increasing pump power and we speculate it caused by collision behavior. Meanwhile, the bandwidth of the frequency spectra is broadened by the increasing probe power, which can be explained by pulse compression. Based on this finding, the optimal frequency spectrum of THz can be achieved by regulating the probe and pump beam.