Tunable external cavity semiconductor laser incorporating a tunable bragg grating

• US 6,470,036 B1
• Filed: 11/03/2000
• Issued: 10/22/2002
• Est. Priority Date: 11/03/2000
• Status: Active Grant

• Current Assignee: Cidra Corporate Services, Inc.
• Original Assignee: Cidra Sarl (Nordic Cultural & Educational Foundation)
• Inventors: Kersey, Alan D., Bailey, Timothy J., Putnam, Martin A., Davis, Michael A., Sanders, Paul E., Brucato, Robert N., Sirkis, James S.
• Primary Examiner(s): Scott, Jr., Leon
• Application Number:
  US09/705,326
• Time in Patent Office: 718 Days
• Field of Search: 372/20, 372/102, 372/64, 372/6, 372/92, 385/37, 385/12
• US Class Current: 372/20
• CPC Class Codes: H01S 3/1053 Control by pressure or deformation
• CPC Class Codes: H01S 3/1055 one of the reflectors being constituted by a diffraction grating
• CPC Class Codes: H01S 5/02325 Mechanically integrated components on mount members or optical micro-benches
• CPC Class Codes: H01S 5/141 using a wavelength selective device, e.g. a grating or etalon H01S5/146 takes precedence

Abstract

A tunable external cavity semiconductor laser incorporating a tunable Bragg grating, including: a semiconductor gain medium; an elongated tuner housing having a tuner housing head and having a tuner housing foot, the tuner housing head and tuner housing foot being rigidly connected; a span of waveguide having a Bragg grating, for receiving the source light and for providing in turn the reflected light, and having a waveguide head and a waveguide foot, the waveguide head abutting the tuner housing head and the waveguide foot disposed toward the tuner housing foot; a piezoelectric crystal or other device or arrangement for providing a compressive force, disposed so as to abut the waveguide foot and also to abut the tuner housing foot, the means for applying a compressive force for exerting a compressive force on the span of waveguide along the direction of the axis of the span of waveguide, the compressive force being sufficient to alter the grating so as to affect the wavelength of light reflected by the grating. In some applications, the waveguide includes sections of different thicknesses, each having a sampled grating, the two sampled gratings being created so that at any given compressive force exerted by the piezoelectric crystal, the two gratings reflect at most one wavelength in common. The tunable laser in such an application therefore behaves as a stepped tunable laser.

Claims

1. A tunable laser system, comprising:

a) a semiconductor gain medium, for providing source light, responsive to reflected light at a reflected wavelength, the gain medium including a lasing material for amplifying the reflected light, and further for providing amplified reflected light;

b) an elongated tuner housing having a tuner housing head and having a tuner housing foot, the tuner housing head and tuner housing foot being rigidly connected;

c) a span of waveguide having a Bragg grating, the waveguide being a large-diameter waveguide so as to be able to respond to a compressive force applied along its longitudinal axis without significant buckling, the span of waveguide for receiving the source light and for providing in turn the reflected light, and having a waveguide head and a waveguide foot, the waveguide head abutting the tuner housing head and the waveguide foot disposed toward the tuner housing foot; and

d) means for applying a compressive force, disposed so as to abut the waveguide foot and also to abut the tuner housing foot, responsive to a controller signal indicating the compressive force to be exerted on the span of waveguide along the direction of the longitudinal axis of the span of waveguide, the compressive force being sufficient to alter the Bragg grating so as to affect the wavelength of light reflected by the Bragg grating.

2. A tunable laser system as in claim 1, wherein the semiconductor gain medium is integrated into the waveguide head of the span of waveguide.

3. A tunable laser system as in claim 1, wherein the semiconductor gain medium is disposed so as to abut the outside of the tuner housing head and wherein the tuner housing head has a borehole provided axially therethrough for passage of light from the semiconductor gain medium and from the Bragg grating.

4. A tunable laser system as in claim 1, wherein the semiconductor gain medium is disposed in spaced apart relation to the outside of the tuner housing head, wherein the tuner housing head has a borehole provided axially therethrough for passage of light from the semiconductor gain medium and from the Bragg grating, and wherein the semiconductor gain medium and the waveguide are coupled via at least one lens.

5. A tunable laser system as in claim 4, wherein the lens coupling the semiconductor gain medium and the waveguide is an aspheric lens.

6. A tunable laser system as in claim 4, further comprising a monitor diode coupled to the semiconductor gain medium, the monitor diode for receiving a fraction of the output of the laser light emitted by the tunable laser system, for providing an indication of the power output of the tunable laser system.

7. A tunable laser system as in claim 1, further comprising a controller coupled to the means for applying a compressive force and also further comprising a temperature sensor, coupled to the controller, responsive to the temperature of the grating, the temperature sensor for providing an indication of the grating temperature to the controller, the controller in turn for applying a signal to the means for applying a compressive force based on the grating temperature, thereby providing a temperature-compensated tunable laser system.

8. A tunable laser system as in claim 1, wherein the means for providing a compressive force is a piezoelectric crystal, responsive to an electric voltage.

9. A tunable laser system as in claim 1, wherein the means for providing a compressive force is a plate in compressive contact with a screw, the screw being advanced or retarded under the influence of a motor, thereby varying the compressive force on the span of waveguide along the direction of the axis of the span of waveguide.

10. A tunable laser system as in claim 1, wherein the means for providing a compressive force is a pair of wedges, including a stationary wedge and a pushing wedge, the pushing we disposed relative to a motor and a motor arm so as to move under the influence of the motor and motor arm more or less into line with the stationary wedge, thereby varying the compressive force on the span of waveguide along the direction of the axis of the span of waveguide.

11. A tunable laser system, comprising:

a) a semiconductor gain medium, for providing source light, responsive to reflected light at a reflected wavelength, the gain medium including a lasing material for amplifying the reflected light, and further for providing amplified reflected light;

b) an elongated tuner housing having a tuner housing head and having a tuner housing foot, the tuner housing head and tuner housing foot being rigidly connected;

c) a span of waveguide having a first sampled grating in a first section of the waveguide for receiving the source light, having a second sampled grating in a second section of the waveguide for receiving the source light, the two gratings having a different sample period, both gratings for providing in turn the reflected light, both sections of the waveguide being of large-diameter so as to be able to respond to a compressive force applied along its longitudinal axis without significant buckling, the span of waveguide also having a waveguide head and a waveguide foot, the waveguide head abutting the tuner housing head and the waveguide foot disposed toward the tuner housing foot; and

d) means for applying a compressive force, disposed so as to abut the waveguide foot and also to abut the tuner housing foot, responsive to a controller signal indicating the compressive force to be exerted on the span of waveguide along the direction of the axis of the span of waveguide;

wherein the first section and second section are of different thicknesses, and the sampled gratings are inscribed in the two sections so that at any given compressive force exerted by the means for applying a compressive force, both gratings reflect at most one common wavelength.