Acoustooptic modulator used for femtosecond laser
A technology of acousto-optic modulator and acousto-optic deflector, applied in instrumentation, optics, nonlinear optics, etc., can solve problems such as spatial and temporal dispersion
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example 1
[0049] As shown in Figure 11, the collimated laser light (800nm) emitted from the laser device 7 passes through the first and second acousto-optic deflectors 5 and 6 with a working frequency of 96 MHz and hits the white screen 9, and is observed and recorded by the CCD 8. Lower the position, change the wavelength of the laser (710nm), at this time the laser cannot pass through the system, there is no light point on the white screen 9, change the operating frequency of the two acousto-optic deflectors to 108.2MHz, and use the CCD8 to observe that the laser hits the white screen again 9 in the same position. Change the wavelength of the laser 7 to 990nm. At this time, there is no light point on the white screen. Change the operating frequency of the two acousto-optic deflectors to 77.6MHz. Observe that the laser still hits the same position on the white screen 9 with the CCD 8 . Changing the power of any one or both of these two acousto-optic deflectors can realize the modulatio...
example 2
[0051] According to the principle schematic diagram shown in Figure 13, a beam of femtosecond laser (800nm) with a pulse width of 141fs (as shown in Figure 14a) passes through the first acousto-optic deflector 5, at this time the frequency of the acousto-optic deflector is set to 96MHz, at this time The femtosecond laser is broadened to 345fs (as shown in Figure 14b), and has spatial dispersion. When the femtosecond laser travels a distance L between the two acousto-optic deflectors, the time dispersion is overcompensated, and the overcompensation amount can just offset the first Time dispersion brought by two AODs 6. After the femtosecond laser passes through the second acousto-optic deflector 6, its spatial dispersion is also fully compensated, and the outgoing light has no temporal dispersion, and its pulse width is still 141 fs (as shown in Figure 14c). Use 141fs after complete dispersion compensation and 345fs without dispersion compensation with the same power laser (2mW...
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