1993
DOI: 10.1016/0030-4018(93)90249-5
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Determination of spectral width and chirp of ultrashort light pulses by analysis of second harmonic beam divergence

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Cited by 10 publications
(3 citation statements)
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“…With the measured pulse duration of 23 fs for a sech 2 pulse shape, the value of the time-bandwidth product ∆t∆ν is 0.576, indicating that the laser pulse is not bandwidthlimited [16]. The diverging image of the SH signal observed in the CCD located 25 or 30 cm from the crystal could be evidence of positive chirp [17]. Further investigation and optimization are required.…”
Section: Resultsmentioning
confidence: 99%
“…With the measured pulse duration of 23 fs for a sech 2 pulse shape, the value of the time-bandwidth product ∆t∆ν is 0.576, indicating that the laser pulse is not bandwidthlimited [16]. The diverging image of the SH signal observed in the CCD located 25 or 30 cm from the crystal could be evidence of positive chirp [17]. Further investigation and optimization are required.…”
Section: Resultsmentioning
confidence: 99%
“…of sum-frequency generation. The width of the secondharmonic beam ∆x is proportional to the pulse duration τ , provided the beam diameter d is large enough [2]:…”
Section: Theorymentioning
confidence: 99%
“…Ultrashort light pulse characterization, which in general includes determination of the temporal dependence of the instantaneous frequency (chirp) or, equivalently, spectral phase, is a difficult and complicated task [1][2][3][4][5][6][7][8][9][10][11][12][13]. Our previous theoretical analysis has shown that the well-known nonlinear autocorrelator based on noncolinear second-harmonic generation (SHG) [13], in addition to pulse duration measurements, can provide measurements of the chirp of a fs pulse [2,4,13]. The SHG autocorrelation method has been verified experimentally with femtosecond pulses produced by the Ti:sapphire laser system based on the Colliding Pulse Amplification (CPA) scheme [7].…”
Section: Introductionmentioning
confidence: 99%