Picosecond High-Voltage Pulses Generation Using Low-Temperature (LT) GaAs

1991 ◽  
Vol 241 ◽  
Author(s):  
T. Motet ◽  
J. Nees ◽  
S. Williamson ◽  
G. Mourou

ABSTRACTWe report on the generation of 825 V electrical pulses with 1.4 ps rise time and 4 ps Full-Width-at-Half-Maximum using pulse biased Low-Temperature-grown GaAs photoconductive switch triggered by submicrojoule, 150 fs laser pulses. Dependence of the temporal pulse shape on both the electric field and the optical energy is observed and discussed.

2012 ◽  
Vol 9 (7) ◽  
pp. 1693-1695
Author(s):  
Juozas Adamonis ◽  
Klemensas Bertulis ◽  
Andrius Bičiūnas ◽  
Ramūnas Adomavičius ◽  
Arūnas Krotkus

2002 ◽  
Vol 19 (4) ◽  
pp. 557-559 ◽  
Author(s):  
Lin Wei-Zhu ◽  
Liu Zhi-Gang ◽  
Liao Rui ◽  
Zhang Hai-Chao ◽  
Guo Bing ◽  
...  

1986 ◽  
Vol 4 (1) ◽  
pp. 141-143 ◽  
Author(s):  
R. B. Wilcox

We have compensated for gain saturation in the Nova amplifiers by producing shaped input optical pulses. A silicon switch device generates kilovolt electrical pulses for driving pockels cells. The pulse shape is easily controllable with subnanosecond resolution.


2012 ◽  
Vol 571 ◽  
pp. 491-495 ◽  
Author(s):  
Peng Wei Gong ◽  
Zhe Ma ◽  
Hong Mei Ma ◽  
Chun Tao Yang

Picosecond or subpicosecond electrical pulses can be generated from femtosecond laser excited photoconductive switches, and this technique is an effective method to characterize the rise time of the broadband oscilloscopes recently. In this paper, low temperature grown GaAs (LT-GaAs) is used as the substrate of the photoconductive switch which is excited by the femtosecond laser. After propagating along a coplanar waveguide, the generated terahertz pulses are transferred to a 1.85 mm coaxial cable through a microwave probe. The pulse width is measured in a 70 GHz sampling oscilloscope, the FWHM value is about 7.4 ps.


2005 ◽  
Vol 10 (2) ◽  
pp. 119-136 ◽  
Author(s):  
A. Dement’ev ◽  
A. Jovaiša

Although the laser pulses with durations ranging from nanoseconds to femtoseconds and various pulse shapes are utilized for the Z-scan measurements, the influence of the temporal pulse shape on the measurement results is often neglected. In this paper, we tried to differentiate the influence of the temporal pulse shape on the common Z-scan technique with a small on-axis aperture in two cases: when the pulse peak intensity at the beam waist is known (for relatively long pulses), or when the total pulse energy and full width at half maximum (FWHM) of the correlation functions or FWHM of pulse durations are known (for short pulses).


2013 ◽  
Vol 2013 ◽  
pp. 1-5
Author(s):  
Seong Jin Cho ◽  
Jaekwan Lim ◽  
Sun Hee Yeon ◽  
O. Sang Kwon ◽  
Kwang-Ho Choi ◽  
...  

In a previous study, we found that Primo vessels generate different action potentials in smooth muscles, but this study compared the pulse shape to distinguish the two tissues. Thus, a more sophisticated extracellular experiment was performed in this study using an acetylcholine injection; we then observed changes in the amplitude, FWHM (full width at half maximum), and period to explore Primo vessel function. A third type of pulse was recorded for Primo vessels. We observed fast depolarizing and repolarizing phases for this pulse. Further, its FWHM was 30 ms between smooth muscles and neurons. Acetylcholine affected only the period. The amplitude and FWHM were consistent after injection. Primo-vessels generated action potentials at twice the frequency after injection. From the results, we speculate that Primo-vessels perform a role in transferring signals in a different manner, which may be relevant for acupuncture treatment.


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