35 results about "Hyperbolic metamaterials" patented technology

Implementing a layered hyperbolic metamaterial in a vertical cavity surface emitting laser (VCSEL) to improve thermal conductivity and thermal dissipation thereby stabilizing optical performance. Improvement in the thermal management and power is expected by replacing the distributed Bragg reflector (DBR) mirrors in the VCSEL. The layered metamaterial structure performs the dual function of the DBR and the heat spreader at the same time.

The invention discloses a method for realizing selective wave absorption through using a hyperbolic metamaterial grating. According to the method, on the basis of the hyperbolic dispersion characteristic of a metal-dielectric periodic film stack, with a sub-wavelength grating structure used in combination, the electromagnetic field enhancement effect of the hyperbolic metamaterial grating is utilized to realize the selective absorption enhancement of light absorptivity for TM polarized incident light; on the basis of determining metal and dielectric material parameters, grating ridge width, metal film layer thickness, dielectric film layer thickness and a film stack number are optimized, the selective absorption enhancement of the light absorptivity under different wave bands can be realized; and the grating ridge width can be adjusted, so that the selection of an absorption peak position can be achieved; and the selective absorption characteristic of the structure is insensitive to the metal-dielectric film stack number, and therefore, the method has high experimental tolerance. Therefore, the method of the present invention has a bright application prospect in fields such as enhanced nano imaging, stealth materials, optoelectronic detection and biosensing. A film stack number can be flexibly selected as needed during practical application.

The invention discloses a Cerenkov radiation device and a manufacturing method thereof, and a radiation extraction method. The Cerenkov radiation device comprises a metal cycle nanometer slit structure, a hyperbolic metamaterial structure and an electron-emitting source, wherein the hyperbolic metamaterial structure is arranged on an upper surface of the metal cycle nanometer slit structure; the electron-emitting source is arranged on an upper surface of the hyperbolic metamaterial structure; and the electron-emitting source includes an anode, a cathode and a grid electrode. The Cerenkov radiation device does not need a high voltage. A characteristic that a phase velocity of light in the hyperbolic metamaterial structure can be reduced by several orders of magnitudes compared to a velocity in a traditional material is used so that a required electronic flight speed generated by Cerenkov radiation can be greatly reduced; and then production cost generated by the Cerenkov radiation device is decreased and safety performance is increased.

A novel thermal source comprising a semiconductor hyperbolic metamaterial provides control of the emission spectrum and the angular emission pattern. These properties arise because of epsilon-near-zero conditions in the semiconductor hyperbolic metamaterial. In particular, the thermal emission is dominated by the epsilon-near-zero effect in the doped quantum wells composing the semiconductor hyperbolic metamaterial. Furthermore, different properties are observed for s and p polarizations, following the characteristics of the strong anisotropy of hyperbolic metamaterials.

A hyperbolic metamaterial assembly comprising alternating one or more first layers and one or more second layers forming a hyperbolic metamaterial, the one or more first layers comprising an intrinsic or non-degenerate extrinsic semiconductor and the one or more second layers comprising a two-dimensional electron or hole gas, wherein one of in-plane or out-of-plane permittivity of the hyperbolic metamaterial assembly is negative and the other is positive.

The invention belongs to the technical field of metamaterial photonic devices, in particular to a cone-shaped hyperbolic metamaterial photonic structure and a preparation method thereof. The cone-shaped hyperbolic metamaterial photonic structure comprises, from top to bottom in turn, a cone-shaped MoO3/Ag composite layer, an Ag film, a MoO3 dielectric layer and a glass substrate, wherein the MoO3dielectric layer has a thickness of 2nm, the Ag film has a thickness of 300nm, the cone-shaped MoO3/Ag composite layer is composed of 2 to 3 layers of MoO3/Ag, wherein each layer of MoO3/Ag has a MoO3thickness of 20nm and an Ag thickness of 15nm. The invention also relates to a preparation method of the cone-shaped hyperbolic metamaterial photonic structure. The cone-shaped hyperbolic metamaterial photonic structure provided by the invention has good anti-reverse performance in a wide spectrum range of 300-1100nm.

The invention provides an adjustable and controllable heat exchange device construction method and system based on near-field radiation. The adjustable and controllable heat exchange device construction method comprises the steps that S1, a heat exchange device main body part is built, and a temperature monitoring sensor and a voltage regulator are used as test regulation and control sensors; S2,the feedback heat exchange of a heat exchange device is regulated and controlled by regulating and controlling the voltage applied to graphene; S3, the graphene and hyperbolic metamaterial hexagonal boron nitride are selected to build the adjustable and controllable heat exchange device; S4, the adjustable and controllable heat exchange device is built by adopting a near-field heat radiation heatdissipation mechanism; and S5, the near-field distance is controlled, and the adjustable and controllable heat exchange device based on near-field radiation is obtained. According to the adjustable and controllable heat exchange device construction method and system, the graphene voltage is applied for regulation and control, so that selective regulation and control of a near-field wave spectrum can be realized, an electronic component is ensured to work in an optimal temperature range, and the corresponding regulation and control temperature difference can reach 50 DEG C.

The invention provides a natural hyperbolic material-based Cherenkov infrared radiation source and free electron light source, which comprises a natural hyperbolic material layer and an on-chip free electron emission source, and the on-chip free electron emission source comprises an on-chip electron source cathode and an on-chip electron source anode. In this way, the on-chip free electron emission source generates a stable electron beam to excite infrared Cherenkov radiation in the natural hyperbolic material. As the natural hyperbolic material is low in cost, easy to obtain and simple in preparation process, the natural hyperbolic material has remarkable advantages compared with an artificial hyperbolic metamaterial. Meanwhile, the natural hyperbolic material is easy to grow, good in stability and few in defect, and the influence of the material processing technology precision on the device performance can be avoided. And on the basis of a natural dielectric material, the intrinsic loss is lower, so that the corresponding device is higher in radiation power, higher in efficiency and smaller in heat emission. In addition, based on a natural crystal material, layout and arraying are easy to realize, and a possible scheme is provided for a high-power array integrated free electron light source.

A device, system and method for producing enhanced external quantum efficiency (EQE) LED emission are disclosed. The device, system and method include a patterned layer configured to transform surfacemodes into directional radiation, a semiconductor layer formed as a III/V direct band gap semiconductor to produce radiation, and a metal back reflector layer configured to reflect incident radiation. The patterned layer may be one-dimensional, two-dimensional or three-dimensional. The patterned layer may be submerged within the semiconductor layer or within the dielectric layer. The semiconductor layer is p-type gallium nitride (GaN). The patterned layer may be a hyperbolic meta-materials (HMM) layer and may include Photonic Hyper-crystal (PhHc), or may be a low or high refractive index material or may be a metal.

A system, method and device for use as a reflector for a light emitting diode (LED) are disclosed. The system, method and device include a first layer designed to reflect transverse-electric (TE) radiation emitted by the LED, a second layer designed to block transverse-magnetic (TM) radiation emitted from the LED, and a plurality of ITO layers designed to operate as a transparent conducting oxidelayer. The first layer may be a one-dimension (1D) distributed Bragg reflective (DBR) layer. The second layer may be a two-dimension (2D) photonic crystal (PhC), a three-dimension (3D) PhC, and/or a hyperbolic metamaterial (HMM). The 2D PhC may include horizontal cylinder bars, vertical cylinder bars, or both. The system, method and device may include a bottom metal reflector that may be Ag free and may act as a bonding layer.

The invention discloses a planar waveguide type hyperbolic metamaterial and an ultra-small resonant cavity. A planar waveguide is formed by two metal plates in the height direction, two kinds of dielectric sheets are alternately and periodically arranged in the planar waveguide, the dielectric sheets are uniform sheets with sub-wavelength thicknesses, the height of the dielectric sheets is the same with that of the planar waveguide, and a metal wire array is arranged on interfaces of the adjacent dielectric sheets and used for restraining mode coupling. The planar waveguide works in a TE modeand can be homogenized into a waveguide type metamaterial, an equal-frequency curve is a hyperbolic curve, and a large wave vector which is more than ten times that of a free space wave vector is supported; the shape of the equal-frequency curve can be adjusted through matching of geometrical parameters and dielectric constants of dielectric materials, and different opening directions are achieved; and the metalmaterial is suitable for all frequency bands from terahertz to microwaves to radio frequency and optical frequency bands. The metamaterial is low in loss, supports large wave vectors,is flexible and adjustable in equal-frequency curve, and is convenient to integrate in a waveguide loop. The ultra-small resonant cavity is realized by adopting the waveguide type hyperbolic metamaterial.

The invention discloses a design method of a plasma sensor and a sensor prepared by the design method. The method comprises the following steps: firstly, utilizing software simulation calculation to obtain optimal combination parameters of a metal filling ratio rho of a hyperbolic metamaterial and a logarithm Nbi of a metal-dielectric layer; and then combining the hyperbolic metamaterial with a polishing surface of a Kretschmann structure or a side polishing optical fiber by a multilayer film structure with the optimal combination parameters to manufacture a corresponding plasma sensor. Compared with the prior art, the design method provided by the invention has the advantages that the performance parameters of the sensor can be controlled by regulating and controlling the metal filling ratio (rho) of the hyperbolic metamaterial and the logarithm (Nbi) of the metal-dielectric layer, so that the controllability of the performance parameters is realized; the plasma sensor prepared by themethod has the advantages of adjustable wavelength, high sensitivity, high quality factor (FOM), simple manufacturing and the like, and is far better than an existing plasma sensor.

A method for fabricating a hyperbolic metamaterial coating having a near-zero refractive index is disclosed. The direction of propagating light changes by means of generating subwavelength structures that alter the coatings permittivity and permeability. The coating can be deposited on lenses or incorporated into optical devices. This type of metamaterial can be utilized to direct light towards sensors or to collect light efficiently.

The invention discloses a hyperbolic metamaterial perfect matching layer method based on time domain finite difference, and belongs to the field of computational electromagnetic simulation. Comprising the following steps: 1) setting simulation parameters of an FDTD algorithm; 2) determining simulation precision and the number of discrete grids; 3) adding a sine wave source into the hyperbolic medium; 4) updating electric field and magnetic field components; 5) drawing magnetic field distribution, and analyzing stability; and 6) data post-processing: if the result of the field quantity of the magnetic field obtained in the step 5) is not convergent or the error is large, the PML is unstable, and the PML needs to be corrected. The problem that electromagnetic waves propagated in a hyperbolic material have numerical divergence in frequency domain PML simulation of traditional PML and COMSOL is solved, the problem that the frequency domain PML in the time domain traditional PML and COMSOL cannot absorb the electromagnetic waves in the hyperbolic material is solved, high stability is shown, and a numerical result further verifies the effectiveness of a PML improvement technology.

The invention provides an on-chip light source, a preparation method of the on-chip light source and a photoelectronic device. An insulating layer is formed on a substrate, an optical array layer is formed on the insulating layer, an isolating layer is formed on the optical array layer, a two-dimensional material layer is formed on the isolating layer, a dielectric layer is formed on the two-dimensional material layer, and a hyperbolic metamaterial layer is formed on the dielectric layer. When the wavelength of the resonance peak of the photon mode of the optical array layer is equal to the wavelength of the exciton peak of the two-dimensional material layer, the luminous intensity of the two-dimensional material layer is enhanced. In addition, the surface plasmon polaritons of the hyperbolic metamaterial layer can generate a strong coupling effect with the two-dimensional material layer, and the Purcell effect is further enhanced. According to the invention, the hyperbolic metamaterial is utilized to enhance the Purcell effect of the two-dimensional material, so that not only can the luminous intensity of the on-chip light source be remarkably improved, but also high luminous efficiency and high response speed can be realized, the size is small, the structure is compact, high-density integration is easy, and good CMOS integration process compatibility is realized.

An absorber for energy harvesting is provided comprising a structure of a multilayered N-doped Si/Si hyperbolic metamaterial (HMM) integrated with a sub-hole Si grating, wherein the structure has a tunable absorption peak tunable from 4.5 μm to 11 μm through changing the grating parameters.