Optical transitional switch
A hyperbolic metamaterial is provided. The hyperbolic metamaterial includes a substrate and sub-wavelength nanostructures arrayed on the substrate. Each sub-wavelength nanostructure has a decreasing cross-sectional area with increasing height from the substrate and includes dielectric or semi-metallic material layers and metal-insulator transition (MIT) material layers respectively interleaved with the dielectric or semi-metallic material layers. Each MIT material layer and each dielectric or semi-metallic material layer of each sub-wavelength nanostructure has a cross-sectional shape characterized in that current is induced in one or both of the dielectric or semi-metallic material layers and the MIT material layers by exposure to a magnetic field.
1 . A hyperbolic metamaterial, comprising:
a substrate; and
sub-wavelength nanostructures arrayed on the substrate,
wherein each sub-wavelength nanostructure has a decreasing cross-sectional area with increasing height from the substrate and comprises:
dielectric or semi-metallic material layers; and
metal-insulator transition (MIT) material layers respectively interleaved with the dielectric or semi-metallic material layers, and
wherein each MIT material layer and each dielectric or semi-metallic material layer of each sub-wavelength nanostructure has a cross-sectional shape characterized in that current is induced in one or both of the dielectric or semi-metallic material layers and the MIT material layers by exposure to a magnetic field.
2 . The hyperbolic metamaterial according to claim 1 , wherein the hyperbolic metamaterial exhibits first emissivity and reflective behavior at first temperatures and second emissivity exceeding the first emissivity at second temperatures exceeding the first temperatures.
3 . The hyperbolic metamaterial according to claim 1 , wherein each MIT material layer and each dielectric or semi-metallic material layer of each sub-wavelength nanostructure has a split-C cross-sectional shape and each sub-wavelength nanostructure has a similar orientation.
4 . The hyperbolic metamaterial according to claim 1 , wherein each MIT material layer and each dielectric or semi-metallic material layer of each sub-wavelength nanostructure has a split-C cross-sectional shape and the sub-wavelength nanostructures have random orientations.
5 . The hyperbolic metamaterial according to claim 1 , wherein each MIT material layer and each dielectric or semi-metallic material layer of each sub-wavelength nanostructure has a horseshoe cross-sectional shape and each sub-wavelength nanostructure has a similar orientation.
6 . The hyperbolic metamaterial according to claim 1 , wherein each MIT material layer and each dielectric or semi-metallic material layer of each sub-wavelength nanostructure has a horseshoe cross-sectional shape and the sub-wavelength nanostructures have random orientations.
7 . The hyperbolic metamaterial according to claim 1 , wherein MIT material of the MIT material layers comprises at least one or more of vanadium oxide, tungsten oxide, titanium dioxide, molybdenum oxide, doped versions of vanadium oxide, tungsten oxide, titanium dioxide and molybdenum oxide, thermochromic materials that undergo a metal-insulator transition and combinations thereof.
8 . A satellite, comprising:
a heat generating element; and
a hyperbolic metamaterial provided as a radiative structure disposed in thermal communication with the heat generating element, the hyperbolic metamaterial comprising:
a substrate; and
sub-wavelength nanostructures arrayed on the substrate,
wherein each sub-wavelength nanostructure has a decreasing cross-sectional area with increasing height from the substrate and comprises:
dielectric or semi-metallic material layers; and
metal-insulator transition (MIT) material layers respectively interleaved with the dielectric or semi-metallic material layers, and
wherein each MIT material layer and each dielectric or semi-metallic material layer of each sub-wavelength nanostructure has a cross-sectional shape characterized in that current is induced in one or both of the dielectric or semi-metallic material layers and the MIT material layers by exposure to a magnetic field.
9 . The satellite according to claim 8 , wherein the heat generating element comprises a satellite payload.
10 . The satellite according to claim 8 , wherein the hyperbolic metamaterial provided as the radiative structure is aimed in a preferential direction.
11 . The satellite according to claim 8 , wherein the hyperbolic metamaterial exhibits first emissivity and reflective behavior at first temperatures and second emissivity exceeding the first emissivity at second temperatures exceeding the first temperatures.
12 . The satellite according to claim 8 , wherein each MIT material layer and each dielectric or semi-metallic material layer of each sub-wavelength nanostructure has a split-C cross-sectional shape and each sub-wavelength nanostructure has a similar orientation.
13 . The satellite according to claim 8 , wherein each MIT material layer and each dielectric or semi-metallic material layer of each sub-wavelength nanostructure has a split-C cross-sectional shape and the sub-wavelength nanostructures have random orientations.
14 . The satellite according to claim 8 , wherein each MIT material layer and each dielectric or semi-metallic material layer of each sub-wavelength nanostructure has a horseshoe cross-sectional shape and each sub-wavelength nanostructure has a similar orientation.
15 . The satellite according to claim 8 , wherein each MIT material layer and each dielectric or semi-metallic material layer of each sub-wavelength nanostructure has a horseshoe cross-sectional shape and the sub-wavelength nanostructures have random orientations.
16 . The satellite according to claim 8 , wherein MIT material of the MIT material layers comprises at least one or more of vanadium oxide, tungsten oxide, titanium dioxide, molybdenum oxide, doped versions of vanadium oxide, tungsten oxide, titanium dioxide and molybdenum oxide, thermochromic materials that undergo a metal-insulator transition and combinations thereof.
17 . A method of forming a hyperbolic metamaterial, the method comprising:
building up an array of sub-wavelength nanostructures on a substrate,
wherein the building up of each sub-wavelength nanostructure comprises:
depositing a dielectric or semi-metallic material layer with a cross-sectional shape characterized in that current is induced in the dielectric or semi-metallic material layer by exposure to a magnetic field;
depositing a metal-insulator transition (MIT) material layer on the dielectric or semi-metallic material layer with a similar cross-sectional shape as the dielectric or semi-metallic material layer; and
successively repeating the depositing of the dielectric or semi-metallic material layer and the depositing of the MIT material layer with each successive layer having a decreased cross-sectional area.
18 . The method according to claim 17 , wherein the cross-sectional shape and the similar cross-sectional shape is a split-C cross-sectional shape and the building up of each sub-wavelength nanostructure comprises orienting each sub-wavelength nanostructure similarly or at random.
19 . The method according to claim 17 , wherein the cross-sectional shape and the similar cross-sectional shape is a horseshoe cross-sectional shape and the building up of each sub-wavelength nanostructure comprises orienting each sub-wavelength nanostructure similarly or at random.
20 . The method according to claim 17 , wherein MIT material comprises at least one or more of vanadium oxide, tungsten oxide, titanium dioxide, molybdenum oxide, doped versions of vanadium oxide, tungsten oxide, titanium dioxide and molybdenum oxide, thermochromic materials that undergo a metal-insulator transition and combinations thereof.