Bulk optic wavelength division multiplexer

• US 5,119,454 A
• Filed: 05/23/1988
• Issued: 06/02/1992
• Est. Priority Date: 05/23/1988
• Status: Expired due to Term

• Current Assignee: Senshin Capital LLC (Intellectual Ventures LLC)
• Original Assignee: Polaroid Corporation (PLR IP Holdings LLC)
• Inventors: McMahon, Donald H.
• Primary Examiner(s): Gonzalez, Frank
• Application Number:
  US07/197,590
• Time in Patent Office: 1,471 Days
• Field of Search: 350/96.10, 350/96.11, 350/96.12, 350/96.13, 350/96.14, 350/96.15, 350/96.16, 350/162.22, 350/162.23, 350/171, 350/355, 350/356, 350/358, 370/1-4
• US Class Current: 385/49
• CPC Class Codes: G02B 6/2931 Diffractive element operating in reflection
• CPC Class Codes: G02B 6/29358 Multiple beam interferometer external to a light guide, e.g. Fabry-Pérot, etalon, VIPA plate, OTDL plate, continuous interferometer, parallel plate resonator G02B6/29347, G02B6/29349, G02B6/2935, G02B6/29361 take precedence; resonator evanescently coupled to light guide G02B6/29335
• CPC Class Codes: G02B 6/2938 for multiplexing or demultiplexing, i.e. combining or separating wavelengths, e.g. 1xN, NxM
• CPC Class Codes: G02B 6/29395 configurable, e.g. tunable or reconfigurable switching G02B6/35
• CPC Class Codes: G02B 6/29398 Temperature insensitivity
• CPC Class Codes: G02B 6/4246 Bidirectionally operating package structures
• CPC Class Codes: G02F 1/21 by interference
• CPC Class Codes: G02F 2201/30 grating

Abstract

An optical multiplexing/demultiplexing device combines an etalon and weak diffraction grating along with temperature control to finely tune local resonant stations along the etalon to separate and/or combine a plurality of optical signals that are finely spaced in wavelength.

Claims

1. An optical multiplexing/demultiplexing device comprising:

an etalon-like structure consisting of a pair of spaced apart, substantially parallel, highly reflective mirror surfaces at least one of which is partially transparent over a predetermined band of wavelengths;

a weak diffraction grating formed on one of said reflective mirror surfaces;

means for coupling a collimated optical beam, containing a plurality of signals of different wavelength within said predetermined band, into said etalon-like structure so that said optical beam travels from one end of said etalon-like structure to the other by being alternately reflected between said reflective mirror surfaces a multiple number of times and strikes said diffraction grating at a predetermined angle of incidence as it travels lengthwise along said etalon-like structure, said diffraction grating being structured so that, acting by itself, it diffracts a small percentage of said signals in said predetermined band perpendicular to said reflective mirror surfaces each time said optical beam is incident thereto at said predetermined angle of incidence; and

means for locally controlling the optical path length between said reflective mirror surfaces at lengthwise locations along said etalon-like structure corresponding to those places where said signals have been diffracted perpendicular to said reflective surfaces to render said lengthwise locations resonant at one or more preselected wavelengths within said predetermined band of wavelengths, each of said selected wavelengths resonant between said reflective mirror surfaces reflecting therebetween a multiplicity of times with at least a part of the energy therein emerging from said lengthwise locations through said reflecting mirror surface which is partially transparent.

2. The device of claim 1 further including means for coupling the remainder of said beam out of the other end of said etalon for subsequent time.

3. The device of claim 1 wherein said highly reflective mirror surfaces are fabricated to be slightly non parallel to provide a controlled physical difference in path length at said lengthwise locations.

4. The device of claim 1 wherein said means for changing the optical path length between said reflective surfaces comprises means for differentially heating said etalon to change the spacing between said reflecting surfaces.

5. The device of claim 1 wherein said etalon comprises a piece of glass with polished surfaces and wherein said reflecting surfaces of said etalon are opposing polished surfaces of said glass that have been coated for reflection.

6. The device of claim 5 wherein one of said reflection surfaces is shorter than the other to provide clear end sections through which signals can be coupled in and out of said piece of glass.

7. The device of claim 5 wherein said glass is an electro-optic material capable of having its index of refraction changed to locally change the optical path length at said lengthwise locations of said etalon between said reflecting surfaces.

8. The device of claim 7 wherein said electro-optic material is selected from the group consisting of lithium niobate, lithium tantalate, ADP, and KDP.

9. The device of claim 7 wherein said means for changing the optical path length between said reflecting surfaces at said lengthwise locations of said etalon comprise means for locally applying electric fields thereto.

10. The device of claim 9 wherein said electric fields are applied in the direction in which said optical signals propagate through said etalon.

11. The device of claim 9 wherein said electric fields are applied perpendicular to the direction in which said signals propagate through said etalon.

12. The device of claim 1 wherein said grating is blazed.

13. The device of claim 1 wherein said means for coupling said optical signals into said etalon comprise an optical waveguide and a collimating lens which directs said signals onto a portion of one of said reflecting surfaces at a predetermined angle of incidence.

14. The device of claim 2 wherein said means for coupling signals out of said etalon comprise and optical waveguide and a lens for receiving remainder signals from said etalon and focusing them into the end of said waveguide.

15. The device of claim 5 wherein said means for changing the optical path length at said lengthwise locations comprises heaters at opposing ends of said etalon for applying a temperature gradient that varies in a predetermined way across the length of said etalon.

16. The device of claim 1 further including an array of photodetectors each of which is positioned along said lengthwise locations to receive a signal at a predetermined wavelength.

17. The device of claim 1 wherein the reflectivity of said reflection surfaces is on the order of 99% and the diffraction efficiency of said grating is 1%.

18. The device of claim 1 wherein said means for changing the optical path length between said reflective surfaces comprises at least one heating element mounted on one end of said etalon like structure for differentially heating it to controllably change the spacing between said reflecting surfaces.

19. The device of claim 1 wherein the spacing between said reflecting surfaces of said etalon like structure and the width of said collimated optical beam are such that the output emerging from its output side in the form of a wavelength continuum.

20. The device of claim 1 further including means for coupling out the remainder of said collimated input beam for further use after portions of it have been removed and demultiplexed by said device.

21. The device of claim 1 further including means for coupling individual signals of predetermined wavelength into said localized resonant lengthwise locations of said device so that said device can be used for multiplexing purposes.

22. The device of claim 21 further including means for coupling collimated light into or out of it at a second location at a predetermined angle of incidence so that said device is completely reservable in operation as either a multiplexer or demultiplexer.