Abstract: Systems and methods are provided for filtering coherent infrared light from a thermal background for protection of infrared (IR) imaging arrays and detection systems. A Michelson interferometer is used for coherent light filtering. In an implementation, a system includes a fixed mirror, a beam splitter, and a moving mirror which can be controlled translationally, as well as tip/tilt. The Michelson interferometer may be used as an imaging system. For imaging applications, a system may comprise a tunable array of micro-electromechanical systems (MEMS) mirrors. A mid-wave IR interferometer with electronic feedback and MEMS mirror array is provided.

Abstract: Mid-IR light emitting diodes (LEDs) based on type-II quantum dot (QD) active regions grown with monolithically integrated semiconductor metal layers are provided. These LEDs comprise layers of type-II semiconductor (e.g., InGaSb) quantum dots integrated into a pn junction diode (e.g., InAs) grown above a highly doped backplane, such as an n++ InAs backplane, all in the same epitaxial growth. Aspects described herein minimize non-radiate recombination times and significantly increase radiative recombination rates by controlling the emission of the emitting QDs in the near field of an optical metal.

Abstract: A mid-infrared detector that uses a heavily doped material (e.g., indium arsenide) as a backplane to the detector structure to improve detector performance and fabrication cost. The infrared detector includes a substrate and a backplane of heavily doped material consisting of two or more of the following materials: indium, gallium, arsenic and antimony. The backplane resides directly on the substrate. The infrared detector further includes a photodetector (e.g., type-I or type-II strained layer superlattice (SLS) nBn photodetector, type-I or type-II SLS pn junction photodetector, a quantum-dot infrared photodetector, a quantum well infrared photodetector, a homogeneous material pn junction photodetector) residing directly on the backplane. Additionally, the infrared detector may include a metal structure residing directly on the photodetector. In this manner, the absorption of electromagnetic energy in the photodetector is enhanced.

Abstract: Embodiments of the invention provide a resonant circuit including an active material substrate excitable by photon energy. A busline having a single input and a single output is located on the active material substrate. A RF resonator geometry is located on the active material substrate in electrical communication with the busline. Application of photon energy to the active material substrate changes the resonance of the RF resonator geometry at room temperatures. Alternately, a resonant circuit is provided that include a passive material substrate. An active material thin film is located on the passive material substrate. A busline having a single input and a single output and a RF resonator geometry located on the active material thin film. The RF resonator geometry is in electrical communication with the busline. Application of photon energy to the active material thin film changes the resonance of the RF resonator geometry at room temperatures.

Abstract: Systems and methods are provided for filtering coherent infrared light from a thermal background for protection of infrared (IR) imaging arrays and detection systems. A Michelson interferometer is used for coherent light filtering. In an implementation, a system includes a fixed mirror, a beam splitter, and a moving mirror which can be controlled translationally, as well as tip/tilt. The Michelson interferometer may be used as an imaging system. For imaging applications, a system may comprise a tunable array of micro-electromechanical systems (MEMS) mirrors. A mid-wave IR interferometer with electronic feedback and MEMS mirror array is provided.

Abstract: A mid-infrared detector that uses a heavily doped material (e.g., indium arsenide) as a backplane to the detector structure to improve detector performance and fabrication cost. The infrared detector includes a substrate and a backplane of heavily doped material consisting of two or more of the following materials: indium, gallium, arsenic and antimony. The backplane re-sides directly on the substrate. The infrared detector further includes a photodetector (e.g., type-I or type-II strained layer superlattice (SLS) nBn photodetector, type-I or type-II SLS pn junction photodetector, a quantum-dot infrared photodetector, a quantum well infrared photodetector, a homogeneous material pn junction photodetector) residing directly on the backplane. Additionally, the infrared detector may include a metal structure residing directly on the photodetector. In this manner, the absorption of electromagnetic energy in the photodetector is enhanced.

Abstract: Embodiments of the invention provide a resonant circuit including an active material substrate excitable by photon energy. A busline having a single input and a single output is located on the active material substrate. A RF resonator geometry is located on the active material substrate in electrical communication with the busline. Application of photon energy to the active material substrate changes the resonance of the RF resonator geometry at room temperatures. Alternately, a resonant circuit is provided that include a passive material substrate. An active material thin film is located on the passive material substrate. A busline having a single input and a single output and a RF resonator geometry located on the active material thin film. The RF resonator geometry is in electrical communication with the busline. Application of photon energy to the active material thin film changes the resonance of the RF resonator geometry at room temperatures.

Abstract: Embodiments herein are directed to a metamaterial transmission filters including a metamaterial component and a upper medium positioned within proximity of the metamaterial component such that movement of the upper medium changes the resonances and optical transmission, reflection or absorption spectra of the filter. The upper material may be a natural material or a second metamaterial identical or non-identical to the metamaterial component. Embodiments herein are designed to allow both continuous tuning of the optical spectra of the assembly and/or discrete spectral switching.

Abstract: A tunable extraordinary optical transmission (EOT) device wherein the tunability derives from controlled variation of the dielectric constant of a semiconducting material (semiconductor) in evanescent-field contact with a metallic array of sub-wavelength apertures. The surface plasmon resonance wavelength can be changed by changing the dielectric constant of the dielectric material. In embodiments of this invention, the dielectric material is a semiconducting material. The dielectric constant of the semiconducting material in the metal/semiconductor interfacial region is controllably adjusted by adjusting one or more of the semiconductor plasma frequency, the concentration and effective mass of free carriers, and the background high-frequency dielectric constant in the interfacial region. Thermal heating and/or voltage-gated carrier-concentration changes may be used to variably adjust the value of the semiconductor dielectric constant.