Pulse autocorrelation measurement method and measurement device based on domain wall nonlinearity
A measurement device and non-linear technology, applied in the direction of instruments, etc., can solve the problems of large pulse width, crystal matching angle, low conversion efficiency of phase matching bandwidth, and large autocorrelation curve width, etc. It is easy to achieve alignment and improve non-linearity The effect of linear conversion efficiency and strong autocorrelation signal
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Embodiment 1
[0032] Such as figure 1As shown, in this embodiment, the light beam to be measured is divided into two beams, one of which is delayed and the two beams are focused on the domain wall of the periodically polarized nonlinear ferroelectric crystal, thereby generating a corresponding Cerenkov radiation multiplier Frequency, the time-domain overlapping part of the two-way Cherenkov radiation frequency multiplication generates sum-frequency light, that is, an autocorrelation signal, adjusts the delay of one beam of light, and measures the difference between the change of the autocorrelation signal and the change of the delay The relationship of the autocorrelation curve is obtained, so as to obtain the pulse time domain width of the beam to be measured.
[0033] Periodically polarized nonlinear ferroelectric crystals are obtained by the following method: select a Z-cut magnesium-doped lithium niobate wafer with a thickness of 1 mm and a 5% mol doping ratio, and the Z direction is th...
Embodiment 2
[0043] Such as image 3 As shown, this embodiment includes: an entrance diaphragm 1, a beam splitter 2, a first right-angle prism 3, a focusing mirror 4, a second right-angle prism 5, a mobile platform 6, a periodically polarized nonlinear ferroelectric crystal 7, a recording Detector 11 and control system 12, wherein: the light to be measured is incident by the incident diaphragm 1, and is divided into two beams of light by the beam splitter 2, and the two beams of light respectively pass through the first rectangular prisms 3 arranged on both sides of the beam splitter 2 Refraction with the second right-angle prism 5 forms a parallel light beam incident on the focusing mirror 4, the second right-angle prism 5 is arranged on the mobile platform 6 to adjust the time delay of one beam of light, and the focusing mirror 4 focuses the two beams of light On the domain wall of the periodically polarized nonlinear ferroelectric crystal 7 , an autocorrelation signal is generated. The ...
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