A large-area preparation method and processing system of a micro-nano structure surface with tunable periodic morphology
A technology of micro-nano structure and processing system, which is applied in the field of large-area preparation method and processing system of micro-nano structure surface with tunable periodic morphology, which can solve the problem of poor tunability, single micro-nano structure morphology, and difficulty in meeting multi-functional surfaces. Processing requirements and other issues, to achieve the effect of simple device and flexible control
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Embodiment 1
[0046] The wavefront control laser interference processing system includes a laser light source 1, an energy attenuator 2, a beam expander 5, a first, a second, and a third mirror 7, 12, 15, and a first and second beam splitters 6, 8, The first, second, third, and fourth half-wave plates 3, 9, 13, 16, the first, second, third, and fourth polarizers 4, 10, 14, 17, wavefront modulation devices 11, CCD camera 20, precision mobile platform 19 and computer 21, such as figure 1 Shown. The half-wave plate and the polarizer are used to control the energy and polarization state of each beam; the wavefront modulation device is used to control the wavefront of the spatial beam; the precision moving platform is used to position and move the sample; the CCD camera is used to monitor the processing process and detection Processing results. The energy of the laser beam emitted by the laser light source 1 is adjusted to an appropriate value through the energy attenuator 2, where the energy at...
Embodiment 2
[0050] The laser light source 1 is selected as a nanosecond pulsed laser with a wavelength of 355nm, the emitted light is divided into three beams and one beam is purely phase modulated by the deformable mirror 11 ( figure 1 ). The three beams are uniformly distributed in space, and their azimuth angles are all 5°, and the polar angles are (0°, 120°, 240°). The polarization directions of the three beams are (-30°, 135°, 300°). When the three beams of spatial light are not phase modulated, the interference pattern is a uniformly distributed rectangular intensity peak ( image 3 ). When the deformable mirror 11 is used to apply a one-dimensional sinusoidal grating ( image 3 ) Phase modulation, the interference image is adjusted to a non-uniform diamond-shaped intensity peak ( image 3 ), which can be used for non-periodic array lithography processing.
Embodiment 3
[0052] The laser light source 1 is selected as a nanosecond pulsed laser with a wavelength of 355nm. The emitted light is divided into three beams and one beam is amplitude modulated by the digital micromirror array 11 ( figure 1 ). The three beams are uniformly distributed in space, and their azimuth angles are all 5°, and the polar angles are (0°, 120°, 240°). The polarization directions of the three beams are (-30°, 210°, 450°). When the three beams of spatial light are not amplitude modulated, the interference pattern is a uniformly distributed circular Gaussian distribution intensity valley ( Figure 4 ). When the digital micromirror array 11 is used to apply a pattern type ( Figure 4 ) Amplitude modulation, the interference image is adjusted to the intensity valley limited by the pattern ( Figure 4 ), which can be used for photolithographic processing of maskless patterned periodic arrays.
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