Apparatus for producing multi pulse by Dammann grating pair
A Daman grating and multi-pulse technology is applied in the field of devices that generate multi-pulse, can solve problems such as low cost, and achieve the effect of low cost and easy fabrication
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Embodiment 1
[0049] Such as figure 2 As shown, the main grating 1 is a 1×2 reflective Damman grating with a period of 25 μm, and two completely identical 1×2 reflective first-stage Damman gratings 21 and 31 are placed at a distance of 30 cm as compensation gratings; The symmetry axes of the primary Damman gratings 21, 31 are on the normal line of the main grating 1, and the normal directions of the main grating 1 and the primary Damman gratings 21, 31 are parallel. The horizontal distance between the two centers is 2cm. Place the first total reflection mirror 2 and the second total reflection mirror 3 apart from the first-order Damman grating 21,31-35cm;
[0050] The laser pulse with positive chirp is incident on the main grating 1, and its positive and negative first-order diffracted lights are respectively incident on the first-order Damman grating 21, 31; the reflected light is reflected by the first total reflection mirror 2 and the second total reflection mirror 3 , the surface of ...
Embodiment 2
[0052] We can separate the input and output light in another way. Such as image 3 As shown, on the normal line of the main grating 1, that is, along the direction of the incident light, a polarizing dielectric template 4 and a 1 / 4 wave plate 5 that are 45° to the optical path are arranged in sequence, and the polarizing dielectric template 4 is opposite to the 45° incident light P-polarized light is completely transparent, while S-polarized light is completely reflected. If the incident light is p-polarized, the output light will become s-polarized due to passing through the 1 / 4 wave plate 5 twice. The p-polarized light is transmitted, and the s-polarized light is totally reflected at 45°, so that the output light and the input light are separated.
Embodiment 3
[0054] The structures of this embodiment and embodiment 2 are basically the same, as Figure 4As shown, when the diameter Φ of the first total reflection mirror 2 and the second total reflection mirror 3 is constant, the distance s between them and the primary Damman grating 21, 31 is not arbitrary, and if s is too small, it will hinder the main grating 1 diffracted light, so there is a minimum s min =Φctgα; α is the diffraction angle of the positive and negative order of the Damman grating used.
[0055] In the experiment, the input pulse measured by the standard second harmonic frequency resolution optical switch device is a double pulse with a chirp of 0.00031 rad / fs, an input pulse of 88.5 fs, and an output pulse of 46.2 fs, which has obvious pulse compression. By adjusting the first-stage Damman gratings 21, 31, a series of double pulses with different pulse intervals can be obtained.
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