Large-area manufacturing method and processing system for surfaces of micrometer and nanometer structures with tunable periods and tunable morphologies
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, first, second, and third mirrors 7, 12, 15, first, and second beam splitters 6, 8, First, second, third, fourth half-wave plates 3, 9, 13, 16, first, second, third, fourth polarizers 4, 10, 14, 17, wavefront modulation device 11, CCD camera 20, precision mobile platform 19 and computer 21, such as figure 1shown. The half-wave plate and polarizer are used to control the energy and polarization state of each beam; the wavefront modulation device is used to regulate the wavefront of the spatial beam; the precision mobile platform is used to position and move the sample; the CCD camera is used to monitor the process and detect 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, wherein the energy attenuator 2 includes the first half-wave p...
Embodiment 2
[0050] The laser light source 1 is selected as a nanosecond pulsed laser with a wavelength of 355nm, the outgoing light is divided into three beams and one of them is purely phase-modulated by the deformable mirror 11 ( figure 1 ). The three beams of light are evenly distributed in space, their azimuth angles are all 5°, and their polar angles are (0°, 120°, 240°). The polarization directions of the three light beams are (-30°, 135°, 300°) in turn. When the three beams of spatial light are not phase-modulated, the interference pattern is a uniformly distributed rectangular intensity peak ( image 3 ). When using the deformable mirror 11 to apply a one-dimensional sinusoidal grating ( image 3 ) phase modulation, the interference image is modulated into a non-uniform diamond-shaped intensity peak ( image 3 ), which can be used for photolithographic processing of non-periodic arrays.
Embodiment 3
[0052] The laser light source 1 is selected as a nanosecond pulsed laser with a wavelength of 355nm, the outgoing light is divided into three beams and one of them is amplitude modulated by a digital micromirror array 11 ( figure 1 ). The three beams of light are evenly distributed in space, their azimuth angles are all 5°, and their polar angles are (0°, 120°, 240°). The polarization directions of the three beams are (-30°, 210°, 450°) in sequence. When the amplitude modulation of the three beams of spatial light is not performed, the interference pattern is a uniformly distributed circular Gaussian distribution of intensity valleys ( Figure 4 ). When using the digital micromirror array 11 to apply a pattern type ( Figure 4 ) amplitude modulation, the interference image is modulated to pattern-limited intensity valleys ( Figure 4 ), which can be used for photolithographic processing of maskless patterned periodic arrays.
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