Configurable geometric metasurface antenna

Patent metadata

Field	Value
Publication number	US-2023094688-A1
Application number	US-202117481590-A
Country	US
Kind code	A1
Filing date	Sep 22, 2021
Priority date	Sep 22, 2021
Publication date	Mar 30, 2023
Grant date	—

Abstract

A tunable metasurface is provided. The tunable metasurface includes a mirror, a dielectric layer disposed on the mirror, a metallic antenna and a phase change material (PCM) layer. The PCM layer is interposed between the dielectric layer and the metallic antenna. The PCM layer is configured to be amorphous or crystalline. The mirror, the dielectric layer, the metallic antenna and the PCM layer cooperatively form a Fabry Perot cavity in which light incident on the metallic antenna from free space is reflected between the mirror and the metallic antenna. The PCM layer has blanket dimensions relative to those of the metallic antenna such that the Fabry Perot cavity is critically coupled with the free space when the PCM layer is only one of amorphous and crystalline.

First claim

What is claimed is:

1 . A tunable metasurface, comprising:
a mirror; a dielectric layer disposed on the mirror; a metallic antenna; and a phase change material (PCM) layer interposed between the dielectric layer and the metallic antenna and configured to be amorphous or crystalline, the mirror, the dielectric layer, the metallic antenna and the PCM layer cooperatively forming a Fabry Perot cavity in which light incident on the metallic antenna from free space is reflected between the mirror and the metallic antenna, and the PCM layer has blanket dimensions relative to those of the metallic antenna such that the Fabry Perot cavity is critically coupled with the free space when the PCM layer is only one of amorphous and crystalline.

2 . The tunable metasurface according to claim 1 , wherein:
when the PCM layer is amorphous, the metallic antenna exhibits maximal cross-polarized light reflection and minimal co-polarized light reflection, and when the PCM layer is crystalline, the metallic antenna exhibits minimal cross-polarized light reflection and minimal co-polarized light reflection.

3 . The tunable metasurface according to claim 1 , wherein:
when the PCM layer is crystalline, the metallic antenna exhibits maximal cross-polarized light reflection and minimal co-polarized light reflection, and when the PCM layer is amorphous, the metallic antenna exhibits minimal cross-polarized light reflection and minimal co-polarized light reflection.

4 . The tunable metasurface according to claim 1 , wherein the mirror is adjacent to the dielectric layer opposite the PCM layer.

5 . The tunable metasurface according to claim 4 , wherein the dielectric layer comprises oxide and the metallic antenna comprises gold.

6 . The tunable metasurface according to claim 4 , wherein the dielectric layer is about three times as thick as the mirror, about twenty times as thick as the metallic antenna and about seven-two hundred times as thick as the PCM layer.

7 . The tunable metasurface according to claim 1 , wherein the PCM layer is about 1-30 nm thick.

8 . The tunable metasurface according to claim 1 , wherein the metallic antenna forms non-right angles with width and length dimensions of the PCM layer.

9 . A tunable metasurface, comprising:
a mirror; a dielectric layer disposed on the mirror; multiple metallic antennas; and a phase change material (PCM) layer interposed between the dielectric layer and the multiple metallic antennas and configured to be amorphous or crystalline, the mirror, the dielectric layer, the multiple metallic antennas and the PCM layer cooperatively forming a Fabry Perot cavity in which light incident on the multiple metallic antennas from free space is reflected between the mirror and the multiple metallic antennas, and the PCM layer has blanket dimensions relative to each of the multiple metallic antennas such that the Fabry Perot cavity is critically coupled with the free space when the PCM layer is only one of amorphous and crystalline.

10 . The tunable metasurface according to claim 9 , wherein:
the Fabry Perot cavity comprises multiple localized sections, and each of the multiple localized sections has a set of the multiple metallic antennas associated therewith.

11 . The tunable metasurface according to claim 10 , wherein the multiple localized sections are independently switchable between on and off states in which the corresponding section of the PCM layer is amorphous and crystalline, respectively, or in which the corresponding section of the PCM layer is crystalline and amorphous, respectively.

12 . The tunable metasurface according to claim 11 , wherein each of the multiple localized sections are optically or electrically switchable between the on and off states.

13 . The tunable metasurface according to claim 9 , wherein:
when a localized section of the PCM layer is amorphous, a set of the multiple metallic antennas associated with the localized section of the PCM layer exhibit maximal cross-polarized light reflection and minimal co-polarized light reflection, and when the localized section of the PCM layer is crystalline, the set of the multiple metallic antennas associated with the localized section of the PCM layer exhibit minimal cross-polarized light reflection and minimal co-polarized light reflection.

14 . The tunable metasurface according to claim 9 , wherein:
when a localized section of the PCM layer is crystalline, a set of the multiple metallic antennas associated with the localized section of the PCM layer exhibit maximal cross-polarized light reflection and minimal co-polarized light reflection, and when the localized section of the PCM layer is amorphous, the set of the multiple metallic antennas associated with the localized section of the PCM layer exhibit minimal cross-polarized light reflection and minimal co-polarized light reflection.

15 . The tunable metasurface according to claim 9 , wherein the mirror is adjacent to the dielectric layer opposite the PCM layer.

16 . The tunable metasurface according to claim 15 , wherein the dielectric layer comprises oxide and the multiple metallic antennas comprise gold.

17 . The tunable metasurface according to claim 15 , wherein the dielectric layer is about three times as thick as the mirror, about twenty times as thick as each of the multiple metallic antennas and about seven-two hundred times as thick as the PCM layer.

18 . The tunable metasurface according to claim 9 , wherein the PCM layer is about 1-30 nm thick.

19 . The tunable metasurface according to claim 9 , wherein:
the multiple metallic antennas form non-right angles with width and length dimensions of the PCM layer, and one or more of the multiple metallic antennas are transversely oriented with one or more others of the multiple metallic antennas.

20 . A method of operating a tunable metasurface comprising a Fabry Perot cavity with a phase change material (PCM) layer extending beyond metallic antennas and having blanket dimensions relative to each metallic antenna such that the Fabry Perot cavity is critically coupled with free space when the PCM layer is only one of amorphous and crystalline, the method comprising:
independently switching a localized section of the PCM layer on or off with the localized section of the PCM layer amorphous or crystalline, respectively, or with the localized section of the PCM layer crystalline or amorphous, respectively, wherein: when the localized section of the PCM layer is on, associated metallic antennas exhibit maximal cross-polarized light reflection and minimal co-polarized light reflection, and when the localized section of the PCM layer is off, the associated metallic antennas exhibit minimal cross-polarized light reflection and minimal co-polarized light reflection.

Assignees

• IBM

Inventors

• Lai Kafai
• Falk Abram L
• Farmer Damon Brooks
• Cohen Guy M

Classifications

• G02F1/292 Primary

  by controlled diffraction or phased-array beam steering (controlled diffraction for optical switching G02F1/31) · CPC title

• G02F2202/30

  Metamaterials · CPC title