Controlled multi-wavelength etalon

• US 6,323,987 B1
• Filed: 05/14/1999
• Issued: 11/27/2001
• Est. Priority Date: 05/14/1999
• Status: Expired due to Term

• Current Assignee: Avago Technologies International Sales Pte Limited (Broadcom, Inc.)
• Original Assignee: Agere Systems Optoelectronics Guardian Corp (Broadcom, Inc.)
• Inventors: Rinaudo, Dominic Paul, Shakespeare, Walter Jeffrey, Bylsma, Richard Bendicks
• Primary Examiner(s): Epps, Georgia
• Assistant Examiner(s): THOMPSON, TIMOTHY J
• Application Number:
  US09/312,387
• Time in Patent Office: 928 Days
• Field of Search: 359/260, 359/589, 250/201.9, 356/454, 356/346, 356/352, 372/6
• US Class Current: 359/260
• CPC Class Codes: G01J 9/0246 Measuring optical wavelength
• CPC Class Codes: H01S 3/08036 using intracavity dispersive, polarising or birefringent elements
• CPC Class Codes: H01S 5/0617 using memorised or pre-programmed laser characteristics
• CPC Class Codes: H01S 5/0687 Stabilising the frequency of the laser

Abstract

A multi-wavelength etalon suitable for tuning and maintaining the operating frequency of a laser used in an optical communication system is disclosed. The communication system has a representative channel wavelength and a channel spacing. The etalon has a plurality of steps on one of the sides with a step size that is a fraction of the channel spacing. The nominal thickness of the etalon is chosen so that a transmission peak occurs at a wavelength substantially equal to the representative channel wavelength and a next peak occurs at the wavelength of an adjacent channel. The step size is a fraction of the channel separation and is substantially optimized so that a peak or trough in the transmission curve in the region of one step overlaps a steep portion of the transmission curve for one or more other steps.

Claims

1. A multi-wavelength etalon comprising:

a body which is transparent at least in a predetermined range of wavelengths and having first and second outwardly facing and opposing sides, the first side having a surface, the second side having a plurality of steps, each step having a surface substantially parallel to the surface of the first side, the surface of the first side and the surfaces of the steps being at least partially reflective;

the first side and the surface of a particular one of the plurality of steps being separated by a thickness d;

the difference between the thicknesses separating the first side and the surfaces of a pair of adjacent steps defining a step size Δ

d;

the distance d being selected such that a transmission intensity curve of light transmitted through the etalon in the region of the particular step in response to light being applied substantially normal to the first side of the etalon is at a first relative peak when the applied light is of a first wavelength λ

, is at a second adjacent relative peak when the applied light is of a second wavelength λ

+cs; and

wherein the step size Δ

d is less than cs.

2. The etalon of claim 1, wherein the reflectivity of the partially reflective surfaces is between approximately 5% and 95%.

3. The etalon of claim 2, wherein the reflectivity of the partially reflective surfaces is approximately 40%.

4. The etalon of claim 1, wherein peaks of transmission intensity curves indicating the magnitude of light transmitted through the etalon in the region of each of said plurality of steps in response to light being applied substantially normal to the first side of the etalon are offset relative to each other such that a peak in the transmission curve associated with one of said plurality of steps overlaps a relatively steeply sloped portion of a transmission curve associated with another of said plurality of steps.

5. The etalon of claim 4, wherein the body has an index of refraction r and the step size Δ

d for each pair of adjacent steps is approximately equal to λ

/(2*r*n), where n is the number of said plurality of steps.

6. The etalon of claim 1, wherein the first wavelength λ

corresponds to a wavelength of a representative optical communication channel in an optical communications system having a plurality of communication channels, and cs corresponds to the difference in wavelength between the representative channel wavelength and the wavelength of an adjacent optical communication channel.

7. A multi-wavelength air-gap etalon comprising:

first and second body components separated by a gap and being transparent at least in a predetermined range of wavelengths;

the first body component having a first outwardly facing side and a first inwardly facing side;

the second body component having a second outwardly facing side and a second inwardly facing side;

the first inwardly facing side having a plurality of steps, each step having a surface substantially parallel to the second inwardly facing side, the surface of the second inwardly facing side and the surfaces of the steps of the first inwardly facing side being at least partially reflective;

the second inwardly facing side and the surface of a particular one of the plurality of steps of the first inwardly facing side being separated by a gap distance d;

the difference between the gap distances separating the second side and the surfaces of a pair of adjacent steps of the first inwardly facing side defining a step size Δ

d;

the gap distance d being selected such that a transmission intensity curve of light transmitted through the etalon in the region of the particular step in response to light being applied substantially normal to the second inwardly facing side of the etalon is at a first relative peak when the applied light is of a first wavelength λ

, is at a second adjacent relative peak when the applied light is of a second wavelength λ

+cs; and

wherein the step size Δ

d is less than cs.

8. A stepped etalon for use in stabilizing the wavelength of a laser light source producing light for use in an optical communication system, the optical communication system having a first communication channel wavelength of λ

and a channel spacing of cs, the etalon comprising;

a transparent body having an index of refraction r and first and second opposing sides, the first side having a surface, the second side having a plurality of steps, each step having a surface substantially parallel to the first side, the surface of the first side and the surfaces of the steps being partially reflective;

the body having a nominal thickness d separating the first side and the surface of a particular one of the plurality of steps equal to approximately (λ

²+λ

*cs)/(2*r*cs); and

the difference between the thicknesses separating the first side and the surfaces of a pair of adjacent steps defining a step size Δ

d, wherein the step size Δ

d for each pair of adjacent steps is approximately equal to λ

/(2*r*n), where n is the number of said plurality of steps.

9. The etalon of claim 8, wherein the transparent body is comprised of a glass having an index of refraction approximately equal to 1.5 and d is substantially 2 mm.

10. The etalon of claim 9, wherein the step size is less than or equal to approximately 258 nm.

11. The etalon of claim 8, wherein the transparent body is comprised of SiO₂.

12. The etalon of claim 9, wherein the reflectivity of the partially reflective surfaces is between approximately 5% and 95%.

13. The etalon of claim 10, wherein the reflectivity of the partially reflective surfaces is approximately 40%.

14. A multi-wavelength etalon comprising:

a body which is transparent at least in a predetermined range of wavelengths and having first and second outwardly facing and opposing sides, the first side having a surface, the second side having a plurality of steps, each step having a surface substantially parallel to the surface of the first side, the surface of the first side and the surfaces of the steps being at least partially reflective;

the first side and the surface of a particular one of the plurality of steps being separated by a thickness d;

the difference between the thicknesses separating the first side and the surfaces of a pair of adjacent steps defining a step size Δ

d;

the distance d being selected such that a reflection intensity curve of light reflected by the etalon in the region of the particular step in response to light being applied substantially normal to the first side of the etalon is at a first relative peak when the applied light is of a first wavelength λ

, is at a second adjacent relative peak when the applied light is of a second wavelength λ

+cs; and

wherein the step size Δ

d is less than cs.