Optical microcavity

About: Optical microcavity is a research topic. Over the lifetime, 2599 publications have been published within this topic receiving 72125 citations. The topic is also known as: optical microcavities.

Optical waveguides in GaAs-AlGaAs epitaxial layers

Abstract: Optical transmission properties are described for two types of waveguides formed in AlxGa1−xAs–GaAs–Alx Ga1−xAs epitaxial layers. The first consists of long smooth‐walled mesas formed by a masking and etching procedure and the second are obtained using an additional etching step to selectively etch the GaAs layer. The latter structure is potentially useful in forming active devices such as modulators since this structure is self‐masking for contacting of the top layer by conventional evaporation techniques. The waveguide dimensions are typically 1–30 μm wide, [sine wave] 1 μm thick, and several mm in length. The transmission measurements are quite similar for both types of guides with attenuation as low as [inverted lazy s]2 cm−1 in wide ([inverted lazy s]20 μm) guides but with losses increasing with decreasing width. The loss appears to arise from imperfections and compositional inhomogeneities in the epitaxial layers.

Strong exciton-photon coupling in a length tunable optical microcavity with J-aggregate dye heterostructures

Abstract: We report the incorporation of thin films of a cyanine dye J aggregate into a versatile, length tunable, optical microcavity. The dense J-aggregate layers give an optical response that can be modified by embedding them at specific positions within heterostructures of dielectric and metal layers. The microcavities are composed of separate gold mirrors, which can be individually nanopositioned, and give sharp resonant modes in the red/near-infrared region of the spectrum. With the dye layer favorably placed, anticrossing behavior is observed as the cavity modes are successively swept through the absorption resonance. Large Rabi splittings of up to 170meV are achieved at room temperature, agreeing well with predictions from a transfer-matrix model. These strongly coupled microcavities pave the way for microelectromechanical systems-integrated microdevices with tailored nonlinear optical properties.

Optical microcavity resonator system

Abstract: An optical resonator system includes a substrate, and a SPARROW optical waveguide disposed on the substrate for evanescently coupling light into an optical microcavity. The SPARROW waveguide includes a multi-layer dielectric stack formed of alternating high and low refractive index dielectric layers, and a waveguide core disposed on the dielectric stack. The waveguide core has an input end and an output end, and is adapted for transmitting optical radiation incident on the input end to the output end. The optical microcavity is disposed at a distance from the optical waveguide that is sufficiently small so as to allow evanescent coupling of light from the optical waveguide into the optical microcavity. The dielectric stack in the SPARROW waveguide isolates the waveguide core and the microcavity from the substrate, so that an optical coupling efficiency approaching 100% can be obtained.

Microcavity discharge device

Abstract: A microcavity discharge device generates radiation with wavelengths in the range of from 11 to 14 nanometers. The device has a semiconductor plug, a dielectric layer, and an anode layer. A microcavity extends completely through the anode and dielectric layers and partially into the semiconductor plug. According to one aspect of the invention, a substrate layer has an aperture aligned with the microcavity. The microcavity is filled with a discharge gas under pressure which is excited by a combination of constant DC current and a pulsed current to produce radiation of the desired wavelength. The radiation is emitted through the base of the microcavity. A second embodiment has a metal layer which transmits radiation with wavelengths in the range of from 11 to 12 nanometers, and which excludes longer wavelengths from the emitted beam.