Polarized frequency-selective optical source

• US 5,499,256 A
• Filed: 02/14/1995
• Issued: 03/12/1996
• Est. Priority Date: 02/14/1995
• Status: Expired due to Term

• Current Assignee: Gemfire Corp. (Medtronic Plc)
• Original Assignee: Deacon Research
• Inventors: Bischel, William K., Brinkman, Michael J., Deacon, David A. G.
• Primary Examiner(s): Scott, Jr., Leon
• Application Number:
  US08/388,318
• Time in Patent Office: 392 Days
• Field of Search: 372/28, 372/27, 372/20, 372/22, 372/12, 372/64, 372/92, 372/98, 385/2
• US Class Current: 372/28
• CPC Class Codes: H01S 2301/14 Semiconductor lasers with special structural design for lasing in a specific polarisation mode
• CPC Class Codes: H01S 5/026 Monolithically integrated components, e.g. waveguides, monitoring photo-detectors, drivers stabilisation of output H01S5/06
• CPC Class Codes: H01S 5/06236 controlling the polarisation, e.g. TM/TE polarisation switching
• CPC Class Codes: H01S 5/125 Distributed Bragg reflector [DBR] lasers
• CPC Class Codes: H01S 5/141 using a wavelength selective device, e.g. a grating or etalon H01S5/146 takes precedence
• CPC Class Codes: H01S 5/4062 with an external cavity or using internal filters, e.g. Talbot filters
• CPC Class Codes: H01S 5/4087 emitting more than one wavelength

Abstract

A laser cavity configuration employs polarization switching to obtain a high output power in a single transverse spatial mode from an integrated external cavity diode laser device. The structure provides stabilization and rapid tuning of the frequency of the diode laser. An advantage is that an integrated structure provides output of the laser in a waveguide with the correct polarization for subsequent applications while supporting optimal polarization in a solid state active medium. The external cavity diode laser according to the invention is consistent with a planar manufacturing process such that high volume, low cost products can be achieved.

Claims

1. A polarized frequency-selective optical source comprising:

a first optical reflector;

at least a second optical reflector aligned with said first optical reflector to define a resonating structure;

a polarized solid state optical gain medium disposed in said resonating structure to generate first polarized optical energy;

a solid state integrated optical tuning structure in an optical path within said resonating structure optically coupled to said optical gain medium, the optical tuning structure comprising;

a frequency-selective polarization converter having a first port and a second port coupled by a first solid state waveguide, said first port coupled to receive said first polarized optical energy; and

a second solid state optical waveguide coupled to said second port of said polarization converter, said second waveguide supporting only second polarized optical energy, said second polarized optical energy being differently polarized than said first polarized optical energy; and

means for extracting frequency-selected optical energy from the optical path passing through said polarization converter, wherein at a selected optical frequency defined by said integrated optical tuning structure, said first polarized optical energy is substantially converted to said second polarized optical energy in order to produce a low-loss longitudinally-twisted polarization mode of said optical energy in said resonating structure.

2. The apparatus according to claim 1 wherein said second waveguide is fabricated in crystalline material by an annealed proton exchange process, such that said second polarized optical energy is polarized along a specific crystalline axis.

3. The apparatus according to claim 2 wherein the second polarized optical energy is orthogonal to said first polarized optical energy and is specifically TM mode in said electro-optically-active crystalline material cut normal to said specific crystalline axis.

4. The apparatus according to claim 2 wherein the second polarized optical energy is orthogonal to said first polarized optical energy and is specifically TE mode in said electro-optically-active crystalline material cut such that said specific crystalline axis lies in the plane of and transverse of said optical path.

5. The apparatus according to claim 1 wherein said second waveguide is fabricated in optically-transmissive solid material with a weak-guiding configuration insufficient to support guiding of TE-polarized optical energy, such that said second polarized optical energy is TM-polarized.

6. The apparatus according to claim 1 wherein said frequency-selective polarization converter is an electro-optically tunable TE-TM converter disposed to provide polarized optical energy at said second port for electro-optically frequency tuning of a fundamental frequency of optical energy of said gain medium.

7. The apparatus according to claim 1 wherein said polarization converter is an electro-optic switch for switching between a switched polarization state relative to a selected frequency and a nonswitched polarization state such that only optical energy at said selected frequency has its polarization switched to said switched polarization state.

8. The apparatus according to claim 1 further including anti-reflection means between said optical gain medium and said integrated optical tuning structure.

9. A polarized frequency-selective optical amplifier comprising:

a polarized solid state optical gain medium disposed in an optical path;

a solid state integrated optical tuning structure in said optical path and optically coupled to said optical gain medium, the optical tuning structure comprising;

a frequency-selective polarization converter having a first port, a second port and a first solid state waveguide coupling said first port and said second port, said first port coupled to receive first polarized optical energy; and

a second solid state optical waveguide coupled to said second port of said polarization converter, said second waveguide supporting only second polarized optical energy, said polarized optical energy being frequency selected by said polarization converter.

10. The apparatus according to claim 9 wherein said second waveguide is fabricated in crystalline material by an annealed proton exchange process, such that said second polarized optical energy is polarized along a specific crystalline axis.

11. The apparatus according to claim 9 wherein said second waveguide is fabricated in optically-transmissive solid material with a weak-guiding configuration insufficient to support guiding of TE-polarized optical energy, such that said second polarized optical energy is TM-polarized.

12. The apparatus according to claim 9 further including an optical energy reflection means disposed to reflect said optical energy in said optical path to retraverse said optical path.

13. The apparatus according to claim 9 wherein said frequency-selective polarization converter is an electro-optically tunable TE-TM converter disposed to provide polarized optical energy at said second port for electrooptically frequency tuning of a fundamental frequency of optical energy of said gain medium.

14. The apparatus according to claim 9 wherein said polarization converter is an electro-optic switch for switching between a switched polarization state relative to a selected frequency and a nonswitched polarization state such that only optical energy at said selected frequency has its polarization switched to said switched polarization state.

15. A polarized frequency-stabilized nonlinearly- converted optical source comprising:

a first optical reflector;

at least a second optical reflector aligned along an optical path, said optical reflector defining a resonating structure with said first optical reflector;

a polarized optical exciter within said resonating structure for generating optical energy at a fundamental frequency polarized in a first sense transverse to propagation direction;

a frequency-selective waveguide polarization converter having a first port and a second port, said first port coupled to receive said first-sense polarized optical energy from said optical exciter;

an optical polarization means coupled to said second port of said polarization converter;

a nonlinear frequency conversion means disposed along said optical path; and

means for extracting frequency-converted optical energy from said optical path,

wherein said polarized optical energy is frequency selected at said fundamental frequency by said frequency-selective waveguide polarization converter to fall within an acceptance frequency range of said nonlinear frequency conversion means to produce output converted optical energy.

16. The apparatus according to claim 15, wherein said frequency-selective polarization converter is electrically tunable by means of an applied electric field between electrodes, said applied electric field for shifting center frequency of said converter.

17. The apparatus according to claim 16, wherein said frequency-selective polarization converter further includes means for adjusting said applied electric field between electrodes to shift center frequency to the center of said acceptance frequency range.

18. The apparatus according to claim 17 wherein said frequency-selective polarization converter is an electro-optically tunable TE-TM converter disposed to provide TM-polarized optical energy at said second port for electro-optically frequency tuning of a fundamental frequency of optical energy of said exciter for controlled tuning of frequency-converted energy.

19. A polarized frequency-selective optical source comprising:

a polarized optical exciter;

a solid state integrated frequency-selective optical tuning structure having a first port and a second port, said first port coupled to receive polarized optical energy polarized in a first sense from said optical exciter, said integrated optical tuning structure comprising;

a frequency selective polarization converter; and

a polarized waveguide for supporting polarized energy in a second sense, wherein said second-sense polarization is different from said first-sense polarization and wherein said second-sense polarized energy is frequency selected by said optical tuning structure.

20. The apparatus according to claim 19 wherein said polarized waveguide is fabricated in crystalline material by an annealed proton exchange process, such that said second-sense polarization is along a specific crystalline axis.

21. The apparatus according to claim 20, wherein said non-polarized optical gain medium is a semiconductor diode laser element.

22. A polarized frequency-selective optical source comprising:

a first optical reflector;

at least a second optical reflector aligned with said first optical reflector to define a resonating structure;

a polarized solid state optical exciter comprising a nonpolarized optical gain medium and a polarizer disposed in said resonating structure to generate first polarized optical energy;

a solid state integrated optical tuning structure in an optical path within said resonating structure optically coupled to said optical gain medium, the optical tuning structure comprising;

a frequency-selective polarization converter having a first port and a second port coupled by a first solid state waveguide, said first port coupled to receive said first polarized optical energy; and

a second solid state optical waveguide coupled to said second port of said polarization converter, said second waveguide supporting only second polarized optical energy, said second polarized optical energy being differently polarized than said first polarized optical energy; and

means for extracting frequency-selected optical energy from the optical path passing through said polarization converter, wherein at a selected optical frequency defined by said integrated optical tuning structure, said first polarized optical energy is substantially converted to said second polarized optical energy in order to produce a low-loss longitudinally-twisted polarization mode of said optical energy in said resonating structure.