Apple Inc.

University of Illinois

Runyu Zhang

Paul Vannest Braun

Yang Li

Chaohao Wang

Zhibing Ge

J Gary Eden

Tong Chen

Sung-Jin Park

Zhenbin Ge

Xiaokai Li

Xianwei Zhao

Khadijeh Bayat

Avery P Yuen

Alex H Pai

Daryl I Vulis

Peng Sun

Brandon J Hui

Christian Ocier

Shang Wang

Jessica A Krogstad

Jesse P Angle

Pralav P Shetty

Hee Jun Yang

Configurations for a beam deflector metasurface are disclosed. The beam deflector metasurface may include beam deflectors arranged in a repeating, radial pattern of concentric zones. The beam deflector metasurface may be a large area, high numerical aperture metasurface optic with high efficiency when directing light at non-normal angles of incidence. The different concentric zones may direct received light in varying directions with various steepness of angles. The beam deflectors may include pillars that may be the same or different width, height, or shape. The pillars may function as diffractive gratings and the cross-coupling between the pillars may direct the output light. The zones of the beam deflector metasurface may allow for diffusing hot spots and spreading the light evenly over the target area. The beam deflector metasurface may be used for non-imaging applications where the deterioration of focus allows for better efficiency at non-normal input and output angles of incidence. The beam deflectors may be designed for polarization and wavelength sensitivity as well as allowing for multiple processing benefits such as patterning the beam deflectors onto active devices.

Beam deflector metasurface

An electronic device such as a head-mounted device may have a display that displays computer-generated content for a user. The head-mounted device may have an optical system that directs the computer-generated content towards eye boxes for viewing by a user. The optical system may include a spatially addressable adjustable optical component. The adjustable optical component may have first and second electrodes and an electrically adjustable material between the first and second electrodes. The electrically adjustable material may include a transparent conductive material such as indium tin oxide that includes a pattern of segmented trenches configured to provide the transparent conductive material with electrical anisotropy. Contacts may be coupled to the transparent conductive material. Control circuitry can adjust the electrically adjustable material to form a spatially addressable light modulator or adjustable lens.

Display system with localized optical adjustments

An aluminized metallic scaffold for high temperature applications comprises a porous non-refractory alloy structure including a network of interconnected pores extending therethrough. The porous non-refractory alloy structure comprises a transition metal phase and an aluminide phase, and portions of the porous non-refractory alloy structure between interconnected pores have a thickness no greater than about 500 nm. A method of making an aluminized metallic scaffold for high-temperature applications comprises introducing aluminum into a surface of a porous metallic structure at an elevated temperature. The porous metallic structure comprises a transition metal and has a network of interconnected pores extending therethrough, where portions of the porous metallic structure between interconnected pores have a thickness no greater than about 500 nm. As the aluminum is introduced into the surface and diffusion occurs, an aluminide phase is formed, resulting in a porous non-refractory alloy structure comprising the aluminide phase and a transition metal phase.

Aluminized metallic scaffold for high temperature applications and method of making an aluminized metallic scaffold

Non-disperse, periodic microplasmas are generated in a volume lacking interfering structures, such as electrodes, to enable photonic interaction between incident electromagnetic energy and the non-disperse, periodic microplasmas. Preferred embodiments leverage 1D, 2D, 3D and super 3D non-disperse, periodic microplasmas. In preferred embodiments, the non-disperse, periodic microplasmas are elongate columnar microplasmas. In other embodiments, the non-disperse, periodic microplasmas are discrete isolated microplasmas. The photonic properties can change by selectively activating groups of the periodic microplasmas.

Control of electromagnetic energy with spatially periodic microplasma devices

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Urbana, IL, United States of America

Runyu Zhang