2012
DOI: 10.1088/2040-8978/14/7/075202
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Theoretical analysis of ASE contrast improvement with a rapid scanning F–P interferometer in a CPA system

Abstract: The use of a rapid scanning Fabry–Pérot (F–P) interferometer as a scanning spectral filter to improve the amplified spontaneous emission (ASE) contrast in a chirped pulse amplification (CPA) laser is proposed and analyzed numerically. The numerical simulation results show that the ASE contrast can be improved by the rapid scanning Fabry–Pérot interferometer by about two orders, and the transmission efficiency of the chirped pulse can exceed 80% with the synchronizing time jitter ranging from  − 5 to 5 ps. Use … Show more

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Cited by 6 publications
(2 citation statements)
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“…As a result, the SNR can be improved in harsh wireless environments where noise or interference is severe. A similar concept to dynamic RF filtering was proposed to filter out optical chirp pulses and to suppress amplified spontaneous noise through tunable optical filtering in chirped pulse amplification optical systems [42]. However, this concept was not presented for RF applications.…”
Section: Concept Of Dynamic Rf Filtering For Ultrabroadband Rf Smentioning
confidence: 99%
“…As a result, the SNR can be improved in harsh wireless environments where noise or interference is severe. A similar concept to dynamic RF filtering was proposed to filter out optical chirp pulses and to suppress amplified spontaneous noise through tunable optical filtering in chirped pulse amplification optical systems [42]. However, this concept was not presented for RF applications.…”
Section: Concept Of Dynamic Rf Filtering For Ultrabroadband Rf Smentioning
confidence: 99%
“…A number of techniques have been proposed and investigated experimentally over the past 20 years aiming to improve the temporal contrast of high peak power laser systems. These methods include the application of saturable absorbers [12], a nonlinear Sagnac interferometer [13], a double CPA scheme [14], nonlinear birefringence [15], cross-polarization wave generation (XPW) [16], a low-gain optical parametric amplification (OPA) [17], self-diffraction (SD) process [18], secondharmonic generation [19], spatial chirp technique [20], methods based on nonlinear Fourier-filter [21], rapid scanning Fabry-Perot (F-P) interferometer [22], plasma mirrors [23], and picosecondpumped OPCPA (PS-OPCPA) [24]. Among these, XPW, plasma mirrors, and PS-OPCPA are the most promising techniques, which have already been applied combined or independently in several petawatt-class laser facilities around the world [25]- [30].…”
Section: Introductionmentioning
confidence: 99%