Nonlinear optical frequency conversion using metamaterial arrays
US-10054839-B1 · Aug 21, 2018 · US
US10459258B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10459258-B2 |
| Application number | US-201715668297-A |
| Country | US |
| Kind code | B2 |
| Filing date | Aug 3, 2017 |
| Priority date | Aug 3, 2016 |
| Publication date | Oct 29, 2019 |
| Grant date | Oct 29, 2019 |
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A method of designing a meta optical device is provided. The method includes: setting, via a processor, design data for arrangement and dimensions of a nanostructure of the meta optical device, according to a function to be implemented by the meta optical device; obtaining a phase change graph with respect to a change in the dimensions; setting a shape dimension region with phase defect in the phase change graph; and substituting a shape dimension with phase defect, which is included in the shape dimension region with phase defect among the dimensions included in the design data, with a substitution value that is outside the shape dimension region with phase defect. Accordingly, a meta optical device having no phase defect is implemented.
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What is claimed is: 1. A method of designing a meta optical device, the method comprising: setting, via a processor, design data for arrangement and shape dimensions of a nanostructure of the meta optical device, according to a function to be implemented by the meta optical device; obtaining a phase change graph with respect to a change in the shape dimensions; setting a shape dimension region with phase defect in the phase change graph; and substituting a shape dimension with phase defect, which is included in the shape dimension region with phase defect among the dimensions included in the design data, with a substitution value that is outside the shape dimension region with phase defect. 2. The method of claim 1 , wherein the shape dimension region with phase defect corresponds to a region where a sign of a slope in the phase change graph reverses. 3. The method of claim 2 , wherein a range of a dimension included in the shape dimension region with phase defect is defined by an inequality, DMIN_PD<DR_PD<DMAX_PD, a left region of the shape dimension region with phase defect in the phase change graph is a first normal region, and a right region thereof is a second normal region, wherein “DMIN_PD” is a numeral indicating lower limit of the shape dimension region with phase defect, and “DMAX_PD” is a numeral indicating an upper limit of the shape dimension region with phase defect, and wherein DMIN_PD and DMAX_PD are determined such that a first sign of a first slope of a straight line connecting two points of the phase change graph respectively corresponding to DMIN_PD and DMAX_PD, a second sign of a first average slope of the phase change graph in the first normal region, and a third sign of a second average slope of the phase change graph in the second normal region are equal to one another. 4. The method of claim 2 , wherein a range of a dimension included in the shape dimension region with phase defect is defined by an inequality, DMIN_PD<DR_PD<DMAX_PD, a left region of the shape dimension region with phase defect in the phase change graph is a first normal region, and a right region thereof is a second normal region, wherein “DMIN_PD” is a numeral indicating a lower limit of the shape dimension region with phase defect, and “DMAX_PD” is a numeral indicating an upper limit of the shape dimension region with phase defect, and wherein DMIN_PD and DMAX_PD are determined such that a first slope of a straight line connecting two points of the phase change graph respectively corresponding to DMIN_PD and DMAX_PD has a value between a second slope of the phase change graph at DMIN_PD and a third slope of the phase change graph at DMAX_PD. 5. The method of claim 2 , wherein a range of a dimension included in the shape dimension region with phase defect is defined by an inequality, DMIN_PD<DR_PD<DMAX_PD, a left region of the shape dimension region with phase defect in the phase change graph is a first normal region, and a right region thereof is a second normal region, wherein “DMIN_PD” is a numeral indicating a lower limit of the shape dimension region with phase defect, and “DMAX_PD” is a numeral indicating an upper limit of the shape dimension region with phase defect, and wherein DMIN_PD and DMAX_PD are determined such that a first slope of a straight line connecting two points of the phase change graph respectively corresponding to DMIN_PD and DMAX_PD has a value between a first average slope of the phase change graph in the first normal region and a second average slope of the phase change graph in the second normal region. 6. The method of claim 3 , wherein the substitution value is one of DMIN_PD and DMAX_PD. 7. The method of claim 3 , wherein, a plurality of shape dimension with phase defects are substituted with one selected from DMIN_PD and DMAX_PD. 8. The method of claim 3 , wherein at least one substitution value that is substituting for a plurality of shape dimensions with phase defect is adjusted to DMIN_PD when the at least one shape dimension with phase defect is closer to DMIN_PD than to DMAX_PD, and the at least one substitution value is adjusted to DMAX_PD when the at least one shape dimension with phase defect is closer to DMAX_PD than to DMIN_PD. 9. A meta optical device designed by the method of claim 1 . 10. A meta optical device comprising: a support layer; and a plurality of nanostructures provided above the support layer, the plurality of nanostructures being arranged to form a dimension distribution that changes a phase of incident light with a certain regularity based on positions of the plurality of nanostructures, and having dimension values that are less than a wavelength of the incident light, wherein signs of slopes of a phase change graph showing a phase change of the incident light with respect to the dimension values of the plurality of nanostructures are consistent. 11. The meta optical device of claim 10 , wherein the dimension values of the plurality of nanostructures exclude a value included in a shape dimension region with phase defect extracted from the phase change graph of the incident light with respect to the dimension values. 12. The meta optical device of claim 10 , wherein the dimension values of the plurality of nanostructures exclude a value causing resonance or quasi-resonance with respect to the incident light. 13. The meta optical device of claim 10 , wherein the plurality of nanostructures have at least one of a cylindrical shape and a polygonal column shape, and wherein the dimension values comprise at least one of a diameter of a cross-sectional circle of a cylinder and a length of one side of a cross-sectional polygon of a polygonal column. 14. The meta optical device of claim 10 , wherein a protrusion height (t) of the plurality of the nanostructures protruding from the support layer satisfies a condition, λ/(2nswg)<t<λ, and wherein λ is the wavelength of the incident light, and nswg is a refractive index of the plurality of nanostructures. 15. The meta optical device of claim 10 , wherein the phase change of the incident light due to the plurality of nanostructures covers a range of 0 degrees to 360 degrees. 16. The meta optical device of claim 10 , wherein the plurality of nanostructures include one of a dielectric material and a semiconductor material. 17. The meta optical device of claim 10 , wherein a refractive index of the plurality of nanostructures is greater than a refractive index of the support layer. 18. The meta optical device of claim 10 , further comprising a cover layer covering a surface of each of the plurality of nano structures in a form of a shell and having a refractive index that is different from a refractive index of the plurality of nanostructures. 19. The meta optical device of claim 10 , further comprising a cover layer entirely covering the plurality of nanostructures. 20. The meta optical device of claim 18 , wherein the refractive index of the cover layer is substantially equal to a refractive index of the support layer. 21. The meta optical device of claim 18 , further comprising an upper dielectric layer arranged above the cover layer and having a refractive index that is different from the refractive index of the cover layer. 22. The meta optical device of claim 10 , further comprising a lower dielectric layer arranged between the support layer and the plurality of nanostructures. 23. The meta optical device of claim 10 , wherein the plurality of nanostructures com
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