Optical feedback locking of semiconductor lasers

• US 4,907,237 A
• Filed: 10/18/1988
• Issued: 03/06/1990
• Est. Priority Date: 10/18/1988
• Status: Expired due to Fees

• Current Assignee: United States Secretary of Commerce
• Original Assignee: THE GOVERNMENT OF THE UNITED STATES OF AMERICA, AS REPRESENTED BY THE SECRETARY OF COMMERCE
• Inventors: Dahmani, Brahim, Hollberg, Leo W.
• Primary Examiner(s): Scott, Jr., Leon
• Application Number:
  US07/259,088
• Time in Patent Office: 504 Days
• Field of Search: 372/29, 372/18, 372/93, 372/95, 372/92, 372/69, 372/75
• US Class Current: 372/32
• CPC Class Codes: H01S 3/0805 by apertures, e.g. pin-holes or knife-edges
• CPC Class Codes: H01S 3/082 defining a plurality of resonators, e.g. for mode selection or suppression
• CPC Class Codes: H01S 5/065 Mode locking; Mode suppression; Mode selection ; Self pulsating
• CPC Class Codes: H01S 5/0656 Seeding, i.e. an additional light input is provided for controlling the laser modes, for example by back-reflecting light from an external optical component H01S5/14, H01S5/4062 and H01S5/4006 take precedence
• CPC Class Codes: H01S 5/0687 Stabilising the frequency of the laser
• CPC Class Codes: H01S 5/14 External cavity lasers H01S5/18 takes precedence; mode locking H01S5/065
• CPC Class Codes: H01S 5/142 which comprises an additional resonator

Abstract

An optical method and apparatus is disclosed for stabilizing the frequencyf semiconductor lasers. The basic system includes only the optical elements of a conventional semiconductor laser optically coupled to a separate, external resonator having an optical cavity with a particular resonance frequency. The optical geometry is configured such that the output from the resonator is fed back to the laser only when the laser frequency matches or substantially matches the resonance frequency. In other disclosed embodiments, optical electronic feedback loops are used to modulate the laser injection current to stabilize the frequency and to adjust the phase of the optical feedback signal.

Claims

1. A stabilized semiconductor diode laser system comprising:

a semiconductor diode laser that emits a beam along a first axis;

said laser having a laser optical field and a carrier density

an optical resonator means, located external to said laser, having a resonator frequency, and including an input port for receiving said laser beam and an output port through which a beam exits said resonator means, said resonator means for producing an enhanced optical output at said output port only when an optical beam supplied at said input port has a frequency substantially equal or exactly equal to said resonant frequency;

first means for optically coupling at least a portion of said beam to said input port; and

second means for optically coupling said output port to said laser as a positive optical feedback thereto whereby inherent coupling of the laser optical field to the carrier density of said laser results in a locking of the laser output frequency.

2. A semiconductor laser system as claimed in claim 1 and further including a beam splitter for dividing said emitted beam into a sampled beam and a system output beam;

and wherein said first coupling means couples said sampled beam to said input port of said resonator means.

3. A semiconductor laser system as claimed in claim 2 wherein said input and said output port are the same.

4. A semiconductor laser system as claimed in claim 3 wherein said first coupling means and said second coupling means are the same.

5. A semiconductor laser system as claimed in claim 2 wherein said optical resonator means comprises a confocal resonator having an axis of symmetry.

6. A semiconductor laser system as claimed in claim 5 wherein said first means couples said sampled beam to said resonator at an angle to said axis of symmetry of said resonator.

7. A semiconductor laser system as claimed in claim 2 and further including means for changing the phase of the optical output of said resonator means.

8. A semiconductor laser system as claimed in claim 7 wherein said phase changing means comprises means optically coupled to receive optical radiation emitted by said resonator means and to convert said optical radiation into an electronic signal.

9. A semiconductor laser system as claimed in claim 8 wherein said phase changing means comprises a modulation lock means for receiving said electronic signal and for generating a correction signal;

and wherein said second coupling means comprises a direction changing mirror mounted on a piezoelectric transducer means for providing movement of said mirror.

10. A semiconductor laser system as claimed in claim 7 and further including means optically coupled to receive optical radiation emitted by said resonator means for converting said optical radiation into an electronic signal;

and means for changing the laser injection current, said modulating means receiving said electronic signal as an input.

11. A semiconductor laser system as claimed in claim 7 wherein said resonator has four ports and produces a first output beam that contains a reflected portion of said coupled sample beam as well as an interfering component, and a second output beam that contains only a reflected portion of said sample beam;

and wherein said second coupling means only couples said second output beam to said laser and blocks said first output beam.

12. A semiconductor laser system as claimed in claim 7 and further including means for monitoring the noise on an output from said resonator and for generating a correction signal to reduce said noise.

13. A semiconductor laser system as claimed in claim 2 and further including means for monitoring an output from said resonator for a frequency imbalance and for generating a correction signal to reduce said frequency imbalance.

14. A semiconductor laser system as claimed in claim 13 wherein said monitoring and generating means includes an RF heterodyne locking means.

15. A method for stabilizing a semiconductor laser that emits a beam comprising:

splitting off a portion of said emitted beam to provide a sample beam;

coupling said sampled beam to an optical resonator located external to said laser and having a resonant frequency;

coupling the output of said resonator back to said laser as a positive feedback only when the frequency of said laser is equal to or substantially equal to said resonant frequency.