Channel-switched tunable laser for DWDM communications

• US 6,373,872 B2
• Filed: 09/10/2001
• Issued: 04/16/2002
• Est. Priority Date: 10/19/1999
• Status: Expired due to Fees

• Current Assignee: Intel Corporation
• Original Assignee: Sparkolor Corp. (Intel Corporation)
• Inventors: Deacon, David A. G.
• Primary Examiner(s): Davie, James W.
• Assistant Examiner(s): MONBLEAU, DAVIENNE N
• Application Number:
  US09/950,359
• Publication Number:
  US 20020018507A1
• Time in Patent Office: 218 Days
• Field of Search: 372/20, 372/28, 372/32, 372/34, 372/94, 372/96, 372/102, 385/4, 385/5, 385/8, 385/10, 385/14, 385/129, 385/132, 385/37
• US Class Current: 372/34
• CPC Class Codes: G02B 2006/12097 Ridge, rib or the like
• CPC Class Codes: G02B 2006/12107 Grating
• CPC Class Codes: G02B 2006/12109 Filter
• CPC Class Codes: G02B 2006/12119 Bend
• CPC Class Codes: G02B 2006/12164 Multiplexing; Demultiplexing
• CPC Class Codes: G02B 6/12007 forming wavelength selective elements, e.g. multiplexer, demultiplexer
• CPC Class Codes: G02B 6/1228 Tapered waveguides, e.g. integrated spot-size transformers for coupling with fibres G02B6/305
• CPC Class Codes: G02B 6/136 by etching
• CPC Class Codes: G02B 6/4202 for coupling an active element with fibres without intermediate optical elements, e.g. fibres with plane ends, fibres with shaped ends, bundles
• CPC Class Codes: G02B 6/4212 the intermediate optical element being a coupling medium interposed therebetween, e.g. epoxy resin, refractive index matching material, index grease, matching liquid or gel
• CPC Class Codes: G02F 1/0147 based on thermo-optic effects G02F1/132 takes precedence
• CPC Class Codes: G02F 1/065 in an optical waveguide structure
• CPC Class Codes: G02F 1/1326 Liquid crystal optical waveguides or liquid crystal cells specially adapted for gating or modulating between optical waveguides
• CPC Class Codes: G02F 2201/307 Reflective grating, i.e. Bragg grating
• CPC Class Codes: G02F 2202/022 polymeric
• CPC Class Codes: H01S 5/0612 controlled by temperature
• CPC Class Codes: H01S 5/0622 Controlling the frequency of the radiation
• 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 5/50 Amplifier structures not provided for in groups H01S5/02 - H01S5/30

Abstract

Laser source including materials with negative index of refraction dependence on temperature and with temperature independent coincidence between cavity modes and a set of specified frequencies such as DWDM channels in telecommunications applications. The free spectral range may be adjusted to equal a rational fraction of the specified frequency interval. The operating frequency may be defined by a frequency selective feedback element that is thermo-optically tuned by the application of heat from an actuator without substantially tuning the cavity modes. The operating frequency may be induced to hop digitally between the specified frequencies. In a particular embodiment, semiconductor amplifier and polymer waveguide segments form a linear resonator with a thermo-optically tuned grating reflector. In a further embodiment, an amplifier and two waveguides from a tunable grating assisted coupler form a ring resonator. Tuning may also be accomplished by means of applying an electric field across a liquid crystal portion of the waveguide structure within the grating.

Claims

1. A laser apparatus comprising:

an amplifying waveguide segment capable of providing optical gain over a first optical frequency band, said amplifying waveguide segment characterized by a first temperature dependent effective refractive index with a positive refractive index change with increases of temperature;

a passive intracavity waveguide segment optically coupled to said amplifying waveguide segment for providing a path for optical energy therein, said passive intracavity waveguide segment characterized by a second temperature-dependent effective refractive index with a negative refractive index change with increases of temperature; and

a frequency selective feedback structure coupling optical energy of a selected second optical frequency band within said first optical frequency band back into said amplifying waveguide segment forming a resonant cavity, wherein said frequency selective feedback structure comprises a thermo-optical feedback waveguide segment, a grating formed in said feedback waveguide segment, and a thermal actuator for heating said feedback waveguide segment to produce a change in refractive index of said feedback waveguide segment for tuning said selected second optical frequency band, and

wherein a round trip optical path traversed by said optical energy within said resonant cavity between successive couplings into said amplifying waveguide segment has a round trip optical length that is substantially independent of ambient temperature over a specified ambient temperature range.

2. The laser apparatus of claim 1 wherein said specified ambient temperature range comprises 5°

C.

3. The laser apparatus of claim 1 wherein said round trip optical length varies by less than ten microns over said specified ambient temperature range.

4. The laser apparatus of claim 1 wherein said passive intracavity waveguide segment comprises a core material having a core refractive index and a cladding material having a cladding refractive index lower than said core refractive index, said core material characterized by a positive refractive index change with temperature increases and said cladding material characterized by a negative refractive index change with temperature increases, with the passive intracavity waveguide segment having a negative net effective refractive index change with temperature increases.

5. The laser apparatus of claim 4 wherein said cladding material comprises a polymer.

6. A laser apparatus of claim 1 wherein said round trip optical length defines a free spectral range of said resonant cavity that is a rational fraction of a specified communication frequency channel spacing over a portion of said first optical frequency band.

7. The laser apparatus of claim 1 wherein said resonant cavity is a ring resonator.

8. The laser apparatus of claim 1 wherein said frequency selective structure is a grating coupler for coupling energy between two waveguide segments.

9. The laser apparatus of claim 1 wherein said amplifying waveguide segment, said passive intracavity waveguide segment, and said frequency selective feedback structure are fabricated on a common substrate.

10. A laser apparatus comprising:

an amplifying waveguide segment capable of providing optical gain over a first optical frequency band, said amplifying waveguide segment characterized by a first temperature dependent effective refractive index with a positive refractive index change with increases of temperature;

a passive intracavity waveguide segment optically coupled to said amplifying waveguide segment for providing a path for optical energy therein, said passive intracavity waveguide segment characterized by a second temperature-dependent effective refractive index with a negative refractive index change with increases of temperature; and

a frequency selective feedback structure coupling optical energy of a selected second optical frequency band within said first optical frequency band from said amplifying waveguide segment back into said amplifying waveguide segment forming a resonant cavity,

wherein a round trip optical path traversed by said optical energy within said resonant cavity between successive couplings into said amplifying waveguide segment has a round trip optical length that is independent of ambient temperature over a specified ambient temperature range, wherein said round trip optical length defines a free spectral range of said resonant cavity that is a rational fraction of a specified frequency channel spacing over a portion of said first optical frequency band.

11. The laser apparatus of claim 10 wherein said passive intracavity waveguide segment comprises a core material having a core refractive index and a cladding material having a cladding refractive index lower than said core refractive index, said core material characterized by a positive refractive index change with temperature increases and said cladding material characterized by a negative refractive index change with temperature increases, with the passive intracavity waveguide segment having a negative net effective refractive index change with temperature increases.

12. The laser apparatus of claim 10 wherein said second frequency band of said frequency selective feedback structure is substantially independent of temperature.

13. The laser apparatus of claim 12 wherein said frequency selective feedback structure comprises an electro-optical feedback waveguide segment, a grating formed in said feedback waveguide segment, and an electrode actuator for applying an electric field in said feedback waveguide segment to produce a change in refractive index of said feedback waveguide segment for tuning said selected second optical frequency.

14. The laser apparatus of claim 10 wherein said frequency selective feedback structure comprises a thermo-optical feedback waveguide segment, a grating formed in said feedback waveguide segment, and a thermal actuator for heating said feedback waveguide segment to produce a change in refractive index of said feedback waveguide segment for tuning said selected second optical frequency.

15. The laser apparatus of claim 10 wherein said resonant cavity is a ring resonator.

16. A laser communication device comprising:

a light amplifying medium capable of providing optical gain over a first optical frequency band extending over an optical communications frequency band;

optical feedback means, including a frequency selective structure capable of providing optical feedback to said light amplifying medium of a selected second optical frequency within said first optical frequency band, for defining a resonant cavity including said light amplifying medium said resonant cavity having an effective round trip optical length characterizing a round trip optical path of optical energy within said resonant cavity between successive couplings of said optical energy into said light amplifying medium said effective round trip optical path length of said resonant cavity establishing longitudinal mode frequencies, a subset of said longitudinal mode frequencies coinciding with specified communications channels within said optical communications frequency band; and

an intracavity medium optically coupled to said light amplifying medium in said round trip optical path of optical energy within said resonant cavity, said intracavity medium characterized by a negative refractive index change with increases in temperature and having a length chosen such that said effective round trip optical length is substantially independent of temperature over a specified temperature range.

17. The device of claim 16 wherein said frequency selective structure comprises a grating structure.

18. The device of claim 17 wherein said frequency selective structure comprises a thermo-optical feedback element, and

a thermal actuator for heating said feedback element to produce a change in refractive index of said feedback element for tuning said selected second optical frequency to a specified communication channel frequency.

19. The device of claim 17 wherein said selected second optical frequency of said frequency selective structure is substantially independent of temperature.

20. The laser apparatus of claim 19 wherein said frequency selective structure comprises an electro-optical feedback element, and

an electrode actuator for applying an electric field in said feedback element to produce a change in refractive index of said feedback element for tuning said selected second optical frequency to a specified communication channel frequency.

21. The device of claim 17 wherein said grating structure is formed on a second waveguide segment coupled to said optical path in s aid cavity.

22. The device of claim 16 wherein said resonant cavity is a ring resonator.

23. A laser apparatus comprising:

an amplifying waveguide segment capable of providing optical gain over a first optical frequency band, said amplifying waveguide segment characterized by a first temperature dependent effective refractive index with a positive refractive index change with increases of temperature;

first and second intracavity waveguide segments optically coupled to opposite ends of said amplifying waveguide segment for providing a path for optical energy therein, at least one of said passive intracavity waveguide segments characterized by a second temperature-dependent effective refractive index with a negative refractive index change with increases of temperature; and

a frequency selective feedback structure coupling optical energy of a selected second optical frequency band within said first optical frequency band between said first and second passive intracavity waveguide segments forming a ring resonant cavity,

wherein a round trip optical path traversed by said optical energy within said ring resonant cavity between successive couplings into said amplifying waveguide segment has a round trip optical length that is substantially independent of ambient temperature over a specified ambient temperature range, wherein said round trip optical length defines a free spectral range of said resonant cavity that is a rational fraction of a specified communication frequency channel spacing over a portion of said first optical frequency band.

24. The laser apparatus of claim 23 wherein said specified ambient temperature range comprises 5°

C.

25. The laser apparatus of claim 23 wherein said first and second passive intracavity waveguide segments comprises a core material having a core refractive index and a cladding material having a cladding refractive index lower than said core refractive index, said core material characterized by a positive refractive index change with temperature increases and said cladding material of at least one of said waveguide segments is characterized by a negative refractive index change with temperature increases, with said at least one passive intracavity waveguide segment having a negative net effective refractive index change with temperature increases.

26. The laser apparatus of claim 25 wherein said cladding material comprises a polymer.

27. The laser apparatus of claim 23 wherein said frequency selective feedback structure comprises a pair of feedback waveguide segments coupled to said first and second passive intracavity waveguide segments, with at least one of said pair being a thermo-optical feedback waveguide segment, a reflective grating formed in said pair of feedback waveguide segment, and a thermal actuator for heating said feedback waveguide segment to produce a change in refractive index of said thermo-optic feedback waveguide segment for tuning said selected second optical frequency.

28. The laser apparatus of claim 23 wherein said frequency selective means comprises a forward coupling grating, having a first waveguide coupled to said first waveguide segment at a first and of said grating and a second waveguide coupled to said second waveguide segment at a second end of said grating, said first and second waveguides having different propagation constants and said grating characterized by a wavenumber matched to the difference in propagation constants between the two waveguides.

29. The laser apparatus of claim 23 wherein one of said first and second waveguides is characterized by a negative refractive index change with increases in temperature and has heating means associated therewith for tuning said frequency selective means.

30. The laser apparatus of claim 29 wherein the other of said first and second waveguides is characterized by a substantially equal and opposite positive refractive index change with increases in temperature and also has heating means associated therewith.

31. The laser apparatus of claim 28 wherein said laser gain medium has heating means operated in coordination with said heating means associated with said forward coupling grating.