2014
DOI: 10.1070/qe2014v044n01abeh015224
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Scanning cross-correlator for monitoring uniform 3D ellipsoidal laser beams

Abstract: The specific features of experimental implementation of a cross-correlator with a scan rate above 1600 cm s-1 and a spatial delay amplitude of more than 15 mm are considered. The possibility of measuring the width of femtosecond pulses propagating in a train 300 ms in duration with a repetition rate of 1 MHz is demonstrated. A time resolution of 300 fs for the maximum time window of 50 ps is attained. The cross-correlator is aimed at testing 3D pulses of a laser driver of an electron photo-injector.

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Cited by 23 publications
(7 citation statements)
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“…The first part is stretched in a fiber Bragg grating stretcher and amplified in a fiber amplifier to an energy of tens of nanojoules, after which it is divided into three replicas. To accurately adjust the time delay, each replica has delay lines based on a piezoelectric disk, which mechanically stretches out the fiber coiled and glued on its side [ 36 ] (not shown in Figure 3) when a proper voltage is applied to the disk. Two replicas are used in ytterbium amplifiers in the solid-state part (Figure 3), and the third one is used as an auxiliary output (point 1.5).…”
Section: Exawatt Center For Extreme Light Studies Lasermentioning
confidence: 99%
“…The first part is stretched in a fiber Bragg grating stretcher and amplified in a fiber amplifier to an energy of tens of nanojoules, after which it is divided into three replicas. To accurately adjust the time delay, each replica has delay lines based on a piezoelectric disk, which mechanically stretches out the fiber coiled and glued on its side [ 36 ] (not shown in Figure 3) when a proper voltage is applied to the disk. Two replicas are used in ytterbium amplifiers in the solid-state part (Figure 3), and the third one is used as an auxiliary output (point 1.5).…”
Section: Exawatt Center For Extreme Light Studies Lasermentioning
confidence: 99%
“…As we mentioned previously, if τ τ F , the intensity distribution in the time domain is proportional to the intensity distribution in the frequency domain. The envelope was recorded by a scanning cross-correlator [40], where we used an oo-e non-collinear second harmonic generation process. The interaction of the shaped operating pulse with the diagnostic channel pulse, whose duration of 0.2 ps was close to the FTL, was implemented in a 1 mm thick nonlinear BBO crystal.…”
Section: Experimental Shaping Of Quasi-triangular Laser Pulsesmentioning
confidence: 99%
“…By varying the delay we observed different time sections of the studied pulses. The cross-correlator was described in detail in our earlier work [13].…”
Section: Description Of the Experimental Setupmentioning
confidence: 99%