Compound metaoptics for amplitude and phase control of wavefronts

Patent metadata

Field	Value
Publication number	US-11333798-B2
Application number	US-201916502817-A
Country	US
Kind code	B2
Filing date	Jul 3, 2019
Priority date	Jul 6, 2018
Publication date	May 17, 2022
Grant date	May 17, 2022

Abstract

A compound metaoptic is presented. The compound metaoptic is comprised of at least two phase-discontinuous metasurfaces, which can convert an incident light beam to an aperture field with a desired magnitude, phase, and polarization profile. Each of the constitutive metasurfaces is designed to exhibit specific refractive properties, which vary along the metasurface. Furthermore, due to its transmission-based operation, the metaoptic can operate without lenses and be low profile: potentially having a thickness on the order of a few wavelengths or less. A systematic design procedure is also presented, which allows conversion between arbitrary complex-valued field distributions without reflection, absorption or active components. Such compound metaoptics may find applications where a specific complex field distribution is desired, including displaying holographic images and augmented or virtual reality systems.

First claim

What is claimed is:

1. A compound metaoptic, comprising:
a first metasurface is configured to receive electromagnetic radiation incident thereon and spatially separated by a distance from a second metasurface and change the power density distribution of the electromagnetic radiation incident thereon to a target power density distribution at a given distance;
wherein the first metasurface operates to refract the electromagnetic radiation onto the second metasurface without reflection and loss and thereby change the power density distribution of the electromagnetic radiation at surface of the second metasurface to match the target power density distribution;
wherein the second metasurface is spatially separated from the first metasurface by the given distance and configured to receive the refracted electromagnetic radiation from the first metasurface and operates to correct the phase of the electromagnetic radiation to match a target phase distribution or a target polarization distribution;
wherein the first metasurface and the second metasurface exhibit bianisotropic properties.

2. The compound metaoptic of claim 1 wherein the first metasurface and the second metasurface are surfaces textured at a subwavelength scale in relation to wavelength of the electromagnetic radiation incident thereon.

3. The compound metaoptic of claim 1 wherein the first metasurface and the second metasurface are further defined as Huygens' metasurfaces.

4. The compound metaoptic of claim 1 wherein at least one of the first metasurface or the second metasurface is comprised of a series of dielectric gratings separated by dielectric spacers.

5. The compound metaoptic of claim 1 wherein at least one of the first metasurface or the second metasurface is comprised of multiple impedance sheets cascaded in propagation direction of the electromagnetic radiation.

6. The compound metaoptic of claim 1 wherein the distance between the first metasurface and the second metasurface is on the order of wavelength of the electromagnetic radiation incident thereon.

7. The compound metaoptic of claim 1 wherein the distance between the first metasurface and the second metasurface is smaller than the wavelength of the electromagnetic radiation incident thereon.

8. The compound metaoptic of claim 1 wherein the distance between the first metasurface and the second metasurface is larger than the wavelength of the electromagnetic radiation incident thereon.

9. The compound metaoptic of claim 1 further comprises a controller electrically coupled to at least one of the first metasurface or the second metasurface, such that at least one of the first metasurface or the second metasurface is divided into a plurality of unit cells and each unit cell is configured to receive a bias voltage from the controller.

10. The compound metaoptic of claim 1 resides in a three-dimensional holographic display.

11. The compound metaoptic of claim 1 resides in an antenna.

12. The compound metaoptic of claim 1 resides in an imaging system.

Assignees

• Univ Michigan Regents

Inventors

• Raeker Brian
• Grbic Anthony

Classifications

• G03H2240/61

  SLM related parameters, e.g. pixel size · CPC title

• G03H2225/22

  Electrically addressed SLM [EA-SLM] · CPC title

• G02B5/3025

  Polarisers, i.e. arrangements capable of producing a definite output polarisation state from an unpolarised input state (G02B5/3008, G02B5/3016 take precedence) · CPC title

• G03H2001/0216

  Optical components (G03H2001/0224, G03H1/0256 take precedence; corresponding details, see subgroups of G03H2223/00) · CPC title

• G02F2202/30

  Metamaterials · CPC title