IP Library › Granted Patent US 11,245,044
Granted Patent B2
US 11,245,044 · App. 16/919,831 · Granted Feb 8, 2022

Plasmonic field-enhanced photodetector and image sensor

Inventor: Hoon Kim (La Habra, CA)
H01L31/035209H01L27/14623H01L27/14665H01L31/103
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Quick Facts
Patent No.
US 11,245,044
App. No.
16/919,831
Granted
Feb 8, 2022
Kind
B2
Abstract

A plasmonic field-enhanced photodetector is disclosed. The photodetector may generate photocurrent by absorbing surface plasmon polaritons (SPPs) generated by combining surface plasmons (SPs) with photons of a light wave.

Claims (42)

1. A photodetector comprising:

a metal layer that shields incident light and generates surface plasmon polaritons (SPPs);

a light absorbing layer that absorbs the generated SPPs and allows charges excited by the absorbed SPPs and a localized electric field effect to tunnel through an insulation film;

a dielectric including nanoholes in which at least a part of the metal layer is opened and formed over the light absorbing layer; and

a semiconductor layer that induces photocurrent based on an electric field effect of tunneled electrons,

wherein the SPPs are generated by interaction between photons of the shielded incident light and surface plasmons (SPs) generated at an interface between the metal layer and the dielectric,

wherein the photocurrent is generated at the semiconductor layer by absorbing the surface plasmon polaritons (SPPs) at the light absorbing layer, and

wherein the SPPs form localized surface plasmons (LSPs) at edges where the metal layer meets the dielectric, and density of a localized electric field increases per unit area to increase the photocurrent as a size of the nanoholes decreases.

2. The photodetector according to claim 1 , wherein the photocurrent is generated by inducing the photocurrent through tunneling caused by the absorbed SPPs.

3. The photodetector according to claim 1 , wherein the generated SPPs are absorbed into the light absorbing layer through the nanohole.

4. The photodetector according to claim 3 , wherein the nanohole is formed of a material having a greater dielectric constant than air.

5. The photodetector according to claim 3 , wherein the nanohole is formed of a material containing Si 3 N 4 .

6. The photodetector according to claim 1 , wherein the metal layer contains at least one of aluminum (Al), gold (Au), or silver (Ag).

7. The photodetector according to claim 1 , wherein the metal layer is extended from a surface to the light absorbing layer and guides the generated SPPs to the light absorbing layer.

8. An image sensor comprising:

a metal surface;

a metal nanohole array formed on the metal surface; and

a detector array formed at a position corresponding to the metal nanohole array,

wherein the metal surface is configured to shield incident light and generate surface plasmon polaritons (SPPs),

wherein the detector array comprises:

a light absorbing layer that absorbs the generated SPPs and allows charges excited by the absorbed SPPs and a localized electric field effect to tunnel through an insulation film;

a dielectric including nanoholes in which at least a part of the metal surface is opened and formed over the light absorbing layer; and

a semiconductor layer that induces photocurrent based on an electric field effect of tunneled electrons,

wherein the SPPs are generated by interaction between photons of the shielded incident light and surface plasmons (SPs) generated at an interface between the metal surface and the dielectric,

wherein the detector array generates the photocurrent at the semiconductor layer by absorbing the surface plasmon polaritons (SPPs) at the light absorbing layer, and

wherein the SPPs form localized surface plasmons (LSPs) at edges where the metal surface meets the dielectric, and density of a localized electric field increases per unit area to increase the photocurrent as a size of the nanoholes decreases.

9. The image sensor according to claim 8 , wherein the detector array generates the photocurrent by inducing the photocurrent through tunneling caused by the absorbed SPPs.

10. The image sensor according to claim 8 , wherein the metal surface is extended from a surface to the light absorbing layer and guides the generated SPPs to the light absorbing layer.

11. A method of operating a photodetector, the method comprising:

absorbing at a light absorbing layer surface plasmon polaritons (SPPs), the SPPs being generated by combining surface plasmons (SPs) with photons of a light wave; and

generating at a semiconductor layer photocurrent by using the absorbed SPPs,

wherein the SPPs form localized surface plasmons (LSPs) at edges where a metal layer meets a dielectric including nanoholes in which at least a part of the metal layer is opened, and density of a localized electric field increases per unit area to increase the photocurrent as a size of the nanoholes decreases, and

wherein the dielectric is formed over the light absorbing layer.

12. The method according to claim 11 , wherein the generation of photocurrent comprises generating the photocurrent by inducing the photocurrent through tunneling caused by the absorbed SPPs.

13. A method of operating an image sensor, the method comprising:

generating photocurrent by using a metal nanohole array formed on a metal surface and a detector array formed at a position corresponding to the metal nanohole array,

wherein the generation of photocurrent comprises:

absorbing at a light absorbing layer surface plasmon polaritons (SPPs), the SPPs being generated by combining surface plasmons (SPs) formed on the metal surface with photons of a light wave, by the detector array; and

generating at a semiconductor layer the photocurrent by using the absorbed SPPs by the detector array,

wherein the SPPs form localized surface plasmons (LSPs) at edges where the metal surface meets a dielectric including nanoholes in which at least a part of the metal surface is opened, and density of a localized electric field increases per unit area to increase the photocurrent as a size of the nanoholes decreases, and

wherein the dielectric is formed over the light absorbing layer.

14. The method according to claim 13 , wherein the generation of the photocurrent comprises generating the photocurrent by inducing the photocurrent through tunneling caused by the absorbed SPPs.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 24, 2025
From: KIM, HOON, DR.
To: TMRW ELECTRONICS, SARL
Reel/Frame 072672/0352 →
Continuity (2)
Provisional Application 62961029 · Jan 14, 2020
Related Publication 20210217794A1 · Jul 15, 2021
Cited By (2)
US 12,237,430 US 12,641,910