Surface plasmon coupler

• US 4,565,422 A
• Filed: 11/30/1983
• Issued: 01/21/1986
• Est. Priority Date: 11/30/1983
• Status: Expired due to Term

• Current Assignee: GTE Laboratories Incorporated (Lumen Technologies, Inc.)
• Original Assignee: GTE Laboratories Incorporated (Lumen Technologies, Inc.)
• Inventors: Seymour, Robert J., Stegeman, George I.
• Primary Examiner(s): LEE, JOHN D
• Application Number:
  US06/556,862
• Time in Patent Office: 783 Days
• Field of Search: 350/96.19, 350/1.1, 350/286, 350/320
• US Class Current: 385/36
• CPC Class Codes: G02B 5/04 Prisms
• CPC Class Codes: G02B 6/34 utilising prism or grating G02B6/293 takes precedence
• CPC Class Codes: Y10S 359/90 Methods

Abstract

A device for efficiently coupling electromagnetic radiation in the far-infrared and submillimeter spectral regions to surface plasmon waves comprises a prism constructed of a dielectric material, a first layer integrally formed on one face of the prism having an index of refraction which is less than the index of refraction of the prism, and a second overcoat layer formed integrally on the first layer and having an index of refraction which is greater than the index of refraction of the first layer.

Claims

1. A device for the efficient coupling of electromagnetic radiation into surface plasmon waves, particularly in the far-infrared or submillimeter spectral regions, said device comprising;

a prism having multiple faces and constructed of a dielectric material which is substantially transparent in the selected spectral region, a first layer integrally formed on one face of the prism also of a material substantially transparent in the selected spectral region and having an index of refraction which is less than the index of refraction of the prism, and a second overcoat layer integrally formed on said first layer also of a material substantially transparent in the selected spectral region and having an index of refraction which is greater than the index of refraction of the first layer.

2. A device in accordance with claim 1 wherein said prism comprises a material of a high dielectric constant..

3. A device in accordance with claim 2 wherein said prism material comprises germanium.

4. A device in accordance with claim 2 wherein said prism material comprises silicon.

5. A device in accordance with claim 1 wherein said first layer comprises a plastic material.

6. A device in accordance with claim 5 wherein said plastic material comprises polyethylene.

7. A device in accordance with claim 1 wherein said second layer comprises a material having a high dielectric constant.

8. A device in accordance with claim 7 wherein said second layer material comprises germanium.

9. A device in accordance with claim 7 wherein said second layer material comprises silicon.

10. A device in accordance with claim 1 wherein the thickness of said first layer is on the order of the penetration distance of an upper mode into the prism.

11. A device in accordance with claim 10 wherein the thickness of the first layer is dependent on the frequency of said mode, and ranges, in wavelength, from approximately 0.010 to 1.0 centimeter from the far-infrared to the submillimeter regions.

12. A device in accordance with claim 11 wherein said second layer has a thickness on the order of 0.0001 to 0.01 centimeter as a function of the frequency over the said wavelength range.

13. A method of fabricating a surface plasmon coupler to provide for efficient coupling of electromagnetic radiation into surface plasmon waves, particularly in the far-infrared and submillimeter spectral regions, said method comprising the steps of:

providing a prism having multiple faces and constructed of a dielectric material which is substantially transparent in the selected spectral region, integrally forming a first layer on one face of the prism also of a material substantially transparent in the selected spectral region and having an index of refraction which is less than the index of refraction of the prism, and integrally overcoating a second layer on the first layer also of a material substantially transparent in the selected spectral region and having an index of refraction which is greater than the index of refraction of the first layer.