A 250-Watts, 0.5-THz continuous-wave second-harmonic gyrotron

2021 ◽  
pp. 1-1
Author(s):  
Mikhail Yu. Glyavin ◽  
Andrey N. Kuftin ◽  
Mikhail V. Morozkin ◽  
Mikhail D. Proyavin ◽  
Andrey P. Fokin ◽  
...  
2010 ◽  
Vol 38 (6) ◽  
pp. 1150-1159 ◽  
Author(s):  
Antonio C Torrezan ◽  
Seong-Tae Han ◽  
Ivan Mastovsky ◽  
Michael A Shapiro ◽  
Jagadishwar R Sirigiri ◽  
...  

2010 ◽  
Vol 53 (4) ◽  
pp. 237-243 ◽  
Author(s):  
N. P. Venediktov ◽  
V. V. Dubrov ◽  
V. E. Zapevalov ◽  
S. Yu. Kornishin ◽  
A. V. Kotov ◽  
...  

2006 ◽  
Vol 34 (3) ◽  
pp. 524-533 ◽  
Author(s):  
M.K. Hornstein ◽  
V.S. Bajaj ◽  
R.G. Griffin ◽  
R.J. Temkin

2021 ◽  
Vol 11 (15) ◽  
pp. 7122
Author(s):  
Simona Mosca ◽  
Tobias Hansson ◽  
Maria Parisi

Optical frequency comb synthesizers with a wide spectral range are an essential tool for many research areas such as spectroscopy, precision metrology, optical communication, and sensing. Recent studies have demonstrated the direct generation of frequency combs, via second-order processes, that are centered on two different spectral regions separated by an octave. Here, we present the capability of optical quadratic frequency combs for broad-bandwidth spectral emission in unexplored regimes. We consider comb formation under phase-matched conditions in a continuous-wave pumped singly resonant second-harmonic cavity, with large intracavity power and control of the detuning over several cavity line widths. The spectral analysis reveals quite distinctive sidebands that arise far away from the pump, singularly or in a mixed regime together with narrowband frequency combs. Notably, by increasing the input power, the optical frequency lines evolve into widely spaced frequency clusters, and at maximum power, they appear in a wavelength range spanning up to 100 nm. The obtained results demonstrate the power of second-order nonlinearities for direct comb production within a wide range of pump wavelengths.


2010 ◽  
Vol 35 (20) ◽  
pp. 3513 ◽  
Author(s):  
G. K. Samanta ◽  
S. Chaitanya Kumar ◽  
Kavita Devi ◽  
M. Ebrahim-Zadeh

2009 ◽  
Vol 4 ◽  
pp. 011-011 ◽  
Author(s):  
Takashi NOTAKE ◽  
Teruo SAITO ◽  
Yoshinori TATEMATSU ◽  
Akihito FUJII ◽  
Shinya OGASAWARA ◽  
...  

2009 ◽  
Vol 94 (15) ◽  
pp. 151107 ◽  
Author(s):  
Sean J. Wagner ◽  
Barry M. Holmes ◽  
Usman Younis ◽  
Amr S. Helmy ◽  
J. Stewart Aitchison ◽  
...  

2020 ◽  
Author(s):  
Xiaotong Guan ◽  
Wenjie Fu ◽  
Jiayi Zhang ◽  
Dun Lu ◽  
Xiaolei Zheng ◽  
...  

2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Jaka Petelin ◽  
Luka Černe ◽  
Jaka Mur ◽  
Vid Agrež ◽  
Jernej Jan Kočica ◽  
...  

Abstract In this manuscript we present a true pulse-on-demand laser design concept using two different approaches. First, we present a fiber master oscillator power amplifier (MOPA) based quasi-continuous wave (CW) laser, working at high modulation bandwidths, for generation of nanosecond pulses. Second, we present a hybrid chirped pulse amplification (CPA)-based laser, combining a chirped-pulse fiber amplifier and an additional solid-state amplifier, for generation of femtosecond pulses. The pulse-on-demand operation is achieved without an external optical modulator/shutter at high-average powers and flexible repetition rates up to 40 MHz, using two variants of the approach for near-constant gain in the amplifier chain. The idler and marker seed sources are combined in the amplifier stages and separated at the out using either wavelength-based separation or second harmonic generation (SHG)-generation-based separation. The nanosecond laser source is further applied to high throughput processing of thin film materials. The laser is combined with a resonant scanner, using the intrinsic pulse-on-demand operation to compensate the scanner’s sinusoidal movement. We applied the setup to processing of indium tin oxide (ITO) and metallic films on flexible substrates.


2012 ◽  
Vol 622-623 ◽  
pp. 1258-1261
Author(s):  
Hong Bo An ◽  
Bing Hua Su ◽  
Li Hong Niu ◽  
Jun Wen Xue

122mW green emission at 532.3nm with a conversion efficiency of 1.2% was measured by single-pass second-harmonic generation in a 10mm long periodically poled MgO:LiNbO3 (MgO:PPLN) crystal is reported. A continuous-wave Yb-doped fiber laser operating at 1064.6nm with narrow bandwidth of 0.1nm is used as pumping source. The experimental temperature acceptance bandwidth ΔT=4.6°C is a little higher than the simulation data of 4°C. Output power instabilities or variations of the green beam pattern were not observed during experiments. In this work, the optimized efficiency was achieved when the waist located at the center of MgO:PPLN and Rayleigh length equal to its length, and the lens’ location in the system was calculated.


Sign in / Sign up

Export Citation Format

Share Document