Multispectral or Hyperspectral Imaging and Imaging System Based on Birefringent Subwavelength Resonating Structure
US-2018107015-A1 · Apr 19, 2018 · US
US11112642B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11112642-B2 |
| Application number | US-201816613604-A |
| Country | US |
| Kind code | B2 |
| Filing date | May 24, 2018 |
| Priority date | May 25, 2017 |
| Publication date | Sep 7, 2021 |
| Grant date | Sep 7, 2021 |
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The invention relates optical devices, for example pixelated devices such as an optical device having a plurality of coloured pixels, each said pixel comprising a filter structure, the filter structure comprising: a first metallic layer; a dielectric layer over said first metallic layer; and a second metallic layer over said dielectric layer; wherein said second metallic layer comprises a nanostructured metallic layer having a lateral structure with features having at least one characteristic lateral dimension equal to or less than 1 μm, and wherein said second metallic layer is structured to couple light incident on said second metallic layer into at least two absorption modes of the filter structure, one to either side of a target wavelength, such that said filter structure appears coloured at said target wavelength in reflected or transmitted light.
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The invention claimed is: 1. An optical device having a plurality of coloured pixels, each said pixel comprising a filter structure, the filter structure comprising: a first metallic layer; a dielectric layer over said first metallic layer; and a second metallic layer over said dielectric layer; wherein said second metallic layer comprises a nanostructured metallic layer having a lateral structure with features having at least one characteristic lateral dimension equal to or less than 1 μm, and wherein said second metallic layer is structured to couple light incident on said second metallic layer into at least two simultaneously present absorption mode peaks of the filter structure, one to either side of a target wavelength, such that said filter structure appears coloured at said target wavelength in reflected or transmitted light, the optical device further comprising a controllable polarizer in an optical path through the filter structure, wherein the controllable polarizer is configured to select an optical response of the pixel, wherein said selection of the optical response comprises controlling a colour of the pixel; and wherein a dominant mode of a first of said absorption mode peaks comprises a surface plasmon mode, and wherein a dominant mode of a second of said absorption mode peaks comprises a simultaneously present guided mode. 2. An optical device as claimed in claim 1 wherein said nanostructured metallic layer is laterally anisotropic such that said filter structure has a first optical response to a first polarisation of said incident light and a second, different optical response to a second polarisation of said incident light orthogonal to said first polarisation. 3. An optical device as claimed in claim 2 wherein said first optical response comprises appearing at a first colour, and wherein said second optical response comprises appearing at a second, different colour or having a substantial absence of colour. 4. An optical device as claimed in claim 1 , wherein said second metallic layer has a lateral structure defining a 1D grating. 5. An optical device as claimed in claim 4 wherein said 1D grating is different for different pixels of the device such that different pixels exhibit different colours in reflected or transmitted light. 6. An optical device as claimed in claim 1 wherein said second metallic layer has a lateral structure defining a plurality of apertures or islands over a lateral region of a pixel. 7. An optical device as claimed in claim 6 wherein said plurality of apertures or islands comprises a 2D array of metallic islands. 8. An optical device as claimed in claim 6 wherein said lateral structure has a first geometry in a first lateral direction and a second, different geometry in a second orthogonal lateral direction. 9. An optical device as claimed in claim 1 wherein the controllable polariser comprises a region of electrically controllable liquid crystal material. 10. An optical device as claimed in claim 1 wherein said at least one characteristic lateral dimension of the lateral structure changes across the filter structure to control a far-field diffraction pattern of the pixel. 11. An optical device as claimed in claim 1 wherein a thickness of the dielectric layer ( 110 ) is less than 300 nm. 12. An optical device as claimed in claim 11 wherein the thickness of the dielectric layer ( 110 ) is less than 150 nm. 13. A method applied to an optical device, of defining the optical response of an optical filter element of the optical device comprising an optical cavity, the optical cavity comprising a first metallic layer, a dielectric layer over said first metallic layer, and a second metallic layer over said dielectric layer, the method comprising: configuring a structure of the second metallic layer to couple light incident on the optical cavity simultaneously into two different mode peaks of the optical cavity, to absorb said incident light at two different wavelengths, one to either side of a target wavelength, such that said structure appears coloured at said target wavelength in reflected or transmitted light; and controlling a polarisation of said incident light to select said optical response of the optical filer element, wherein said selection of the optical response comprises controlling the colour of the optical filer element; wherein a dominant mode of a first of said absorption mode peaks comprises a surface plasmon mode, and wherein a dominant mode of a second of said absorption mode peaks comprises a simultaneously present guided mode. 14. A method as claimed in claim 13 comprising configuring the second metallic layer as a 1D or 2D array of apertures in a metallic sheet or as a 1D or 2D array of metallic islands. 15. A method as claimed in claim 14 wherein further comprising varying a geometry of said 1D or 2D array over a lateral area of the optical filter element to vary an effective near or far field shape of the optical filter element. 16. A method applied to an optical device, of defining an optical response of an optical filter element of the optical device comprising an optical cavity, the optical cavity comprising a first metallic layer, a dielectric layer over said first metallic layer, and a second metallic layer over said dielectric layer, the method comprising: configuring the second metallic layer as a 1D or 2D array of apertures in a metallic sheet or as a 1D or 2D array of metallic islands to couple light incident on the optical cavity into at least one surface plasmon resonant mode of the optical cavity, and varying a geometry of said 1D or 2D array over a lateral area of the optical filter element to vary an effective near or far field shape of the optical filter element, wherein said configuring comprises configuring a structure of the second metallic layer to couple light incident on the optical cavity simultaneously into two different mode peaks of the optical cavity, to absorb said incident light at two different wavelengths, one to either side of a target wavelength, such that said structure appears coloured at said target wavelength in reflected or transmitted light; and controlling a polarisation of said incident light to select said optical response of the optical filer element, wherein said selection of the optical response comprises controlling the colour of the optical filer element; wherein a dominant mode of a first of said absorption mode peaks comprises a surface plasmon mode, and wherein a dominant mode of a second of said absorption mode peaks comprises a simultaneously present guided mode. 17. A method as claimed in 16 wherein at least one of said modes comprises a surface plasmon resonant mode of said cavity.
Surface plasmon devices (diffractive gratings with a pitch less than or comparable to the wavelength G02B5/1809; surface plasmons in integrated optics G02B6/1226; optical analysis of materials by means of surface plasmons G01N21/553) · CPC title
in the form of arrays · CPC title
Diffractive Fresnel lenses; Zone plates; Kinoforms (G02B5/1842, G02B5/1847 take precedence; optical systems having diffractive correction means G02B27/0037; Fresnel lenses operating by refraction G02B3/08) · CPC title
comprising at least one thin film resonant cavity, e.g. in bandpass filters · CPC title
Colour filters · CPC title
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