Method and apparatus for wavelength tuning laser diodes

• US 20090238217A1
• Filed: 05/23/2008
• Published: 09/24/2009
• Est. Priority Date: 03/21/2008
• Status: Active Grant

• Current Assignee: Coherent Inc (Coherent Corp.)
• Original Assignee: Ondax Incorporated (Coherent Corp.)
• Inventors: Ho, Lawrence Pokwah, Havermeyer, Frank, Moser, Christophe
• Granted Patent: US 7,636,376 B2
• Time in Patent Office: Days
• US Class Current: 372/20
• CPC Class Codes: H01S 3/08059 Constructional details of the reflector, e.g. shape mirrors in general G02B5/08; mountings for mirrors G02B7/18
• CPC Class Codes: H01S 3/1055 one of the reflectors being constituted by a diffraction grating
• 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 5/143 Littman-Metcalf configuration, e.g. laser - grating - mirror
• CPC Class Codes: H01S 5/4062 with an external cavity or using internal filters, e.g. Talbot filters

Abstract

A method is presented for shaping the spectral response of volume holographic grating elements by applying controlled thermal energy. The methods allow generating continuous or discontinuous grating periods from a fixed grating period. The methods are applicable to optical feedback into optical sources such as light emitting diodes, lasers and other general optical filtering applications.

Claims

1. A laser source tunable in wavelength with a degenerate self-aligned external cavity comprising:

an amplifier waveguided medium placed inside the external cavity,

a lens assembly to collimate the light from said waveguide amplifier,

a reflective volume holographic grating element as the output coupler and the wavelength selective component of the external cavity wherein,

said volume holographic grating element has a grating vector substantially non-parallel with respect to the first collimated beam and receives a first and second collimated beam and generates a first and second filtered beam wherein,

the first filtered beam is propagating in a direction opposite and substantially non-parallel with respect to the first collimated beam and the second filtered beam is propagating in a direction opposite and substantially parallel to said first collimated beam and providing optical feedback to said waveguide amplifier,

a mirror positioned adjacent to said waveguide amplifier wherein,

the reflective facet of the mirror is placed at the focal plane of said lens assembly and which receives and reflects said first filtered beam to produce said second collimated beam after collimation from said lens assembly wherein,

said second collimated beam produces said second filtered beam upon diffraction from said volume holographic grating element.

2. The tunable laser of claim 1, wherein the waveguide amplifier medium is a fiber.

3. The tunable laser of claim 1, wherein the waveguide is a single spatial mode semi-conductor laser diode.

4. The tunable laser of claim 1, wherein the waveguide is a broad area semi-conductor laser diode.

5. The tunable laser of claim 1, wherein the waveguide is an array of broad area semi-conductor laser diode.

6. The tunable laser of claim 1, wherein the lens assembly is a combination of a fast axis lens and slow axis lens

7. The tunable laser of claim 1, wherein the lens assembly is any combination of aspherical lenses, achromatic lenses, cylindrical lenses, aspherical cylindrical lenses, ball lenses, grin lenses.

8. The tunable laser of claim 1, wherein the lens assembly is a combination of a fast axis lens and a slow axis lens.

9. The tunable laser of claim 1, wherein the reflective volume holographic grating element is made of photosensitive glass.

10. The tunable laser of claim 1, wherein the reflective volume holographic grating element is rotated around any axis which is neither parallel to said first collimated beam axis nor parallel to grating vector to said holographic grating element.

11. A laser source tunable in wavelength with a degenerate self-aligned external cavity comprising:

an amplifier waveguided medium placed inside the external cavity,

a lens assembly defining an optical axis to collimate the light from the waveguide amplifier to produce a first collimated beam,

a polarizing beam-splitter,

a quarter-wave plate,

a reflective volume holographic grating element as the output coupler and the wavelength selective component of the external cavity wherein

said volume holographic grating element first receives said first collimated beam and generates a plurality of filtered beams propagating in a direction opposite and substantially non-parallel with respect to said first collimated beam,

a reflecting assembly receiving said plurality of filtered beams reflected from said polarizing beam-splitter and producing a second subset of at least one collimated beam after reflection from said polarizing beam-splitter and collimation from said lens assembly wherein,

said second subset of at least one collimated beam produces a second subset of at least one filtered beam upon diffraction from said volume holographic grating element, wherein

second subset of at least one filtered beam propagates in a direction substantially parallel to first collimated beam and produces optical feedback into said amplifier waveguided medium.

12. The tunable laser of claim 11, wherein the waveguide amplifier medium is a fiber.

13. The tunable laser of claim 11, wherein the waveguide is a single spatial mode semi-conductor laser diode.

14. The tunable laser of claim 11, wherein the waveguide is a broad area semi-conductor laser diode.

15. The tunable laser of claim 11, wherein the waveguide is an array of broad area semi-conductor laser diode.

16. The tunable laser of claim 11, wherein the lens assembly is any combination of aspherical lenses, achromatic lenses, cylindrical lenses, aspherical cylindrical lenses, ball lenses, grin lenses.

17. The tunable laser of claim 11, wherein the lens assembly is a combination of a fast axis lens and a slow axis lens.

18. The tunable laser of claim 11, wherein the reflective volume holographic grating element is made of photosensitive glass.

19. The tunable laser of claim 11, wherein the reflective volume holographic grating element contains one of more overlapped reflective volume gratings each with distinct grating vector.

20. The tunable laser of claim 11, wherein the reflective volume holographic grating element is rotated around any axis which is neither parallel to said first collimated beam axis nor parallel to grating vector to said holographic grating element.

21. The tunable laser of claim 11, wherein the reflecting assembly is a mirror element which is either a planar mirror, an array of reflecting liquid crystal cells or an array of micro-mirrors positioned at the focal plane of the lens assembly where said plurality of filtered beams comes into a focus.

22. The tunable laser of claim 11, wherein the reflecting assembly is a retro-reflector corner cube or retro-reflector prism element positioned after first lens assembly.

23. The tunable laser of claim 11, wherein the reflecting assembly is positioned after first lens assembly and wherein,

the reflecting assembly is formed by a second focusing lens and a mirror element, wherein,

the mirror element is either a planar mirror, an array of reflecting liquid crystal cells or an array of micro-mirrors positioned at the focal plane of said second focusing lens where said plurality of filtered beams comes into a focus.

24. A laser source tunable in wavelength with a degenerate self-aligned external cavity comprising:

an amplifier waveguided medium placed inside the external cavity,

a first lens assembly defining an optical axis to collimate the light from the waveguide amplifier to produce a first collimated beam,

a reflective volume holographic grating element as the output coupler and the wavelength selective component of the external cavity wherein,

said volume holographic grating element first receives said first collimated beam and generates a plurality of filtered beams propagating in a direction substantially non-parallel with respect to said first collimated beam,

a reflecting assembly receiving said plurality of filtered beams and producing a second subset of at least one collimated beam wherein,

said second subset of at least one collimated beam produces a second subset of at least one filtered beam upon diffraction from said volume holographic grating element, wherein

second subset of at least one filtered beam propagates in a direction substantially parallel to first collimated beam and produces optical feedback into said amplifier waveguided medium.

25. The tunable laser of claim 24, wherein the waveguide amplifier medium is a fiber.

26. The tunable laser of claim 24, wherein the waveguide is a single spatial mode semi-conductor laser diode.

27. The tunable laser of claim 24, wherein the waveguide is a broad area semi-conductor laser diode.

28. The tunable laser of claim 24, wherein the waveguide is an array of broad area semi-conductor laser diode.

29. The tunable laser of claim 24, wherein the lens assembly is any combination of aspherical lenses, achromatic lenses, cylindrical lenses, aspherical cylindrical lenses, ball lenses, grin lenses.

30. The tunable laser of claim 24, wherein the lens assembly is a combination of a fast axis lens and a slow axis lens.

31. The tunable laser of claim 24, wherein the reflective volume holographic grating element is made of photosensitive glass.

32. The tunable laser of claim 24, wherein the reflective volume holographic grating element contains one of more overlapped reflective gratings each with distinct grating vector.

33. The tunable laser of claim 24, wherein the reflective volume holographic grating element is rotated around an axis orthogonal to the plane defined by said first collimated beam and a grating vector from said reflective volume holographic element.

34. The tunable laser of claim 24, wherein the reflecting assembly is a retro-reflector corner cube or retro-reflector prism element positioned after first lens assembly.

35. The tunable laser of claim 24, wherein the reflecting assembly is positioned after first lens assembly and wherein,

The reflecting assembly is formed by a second focusing lens and a mirror element, wherein,

the mirror element is either a planar mirror, an array of reflecting liquid crystal cells or an array of micro-mirrors positioned at the focal plane of said second focusing lens where said plurality of filtered beams comes into a focus.

36. A second harmonic laser source comprising:

a pump laser diode source,

an amplifier medium whose facet facing said pump laser diode forms one side of the fundamental cavity,

a non-linear material to generate second harmonic light positioned adjacent to said amplifier medium whose facet opposite said amplifier medium is the output coupler of the fundamental cavity,

a first lens assembly to collimate the light from said pump laser diode,

a reflective volume holographic grating element as the output coupler of the external cavity of said pump laser diode source and the wavelength selective component of the pump external cavity wherein

said grating element receives a first and second collimated beam from said laser diode pump and generates a first and second filtered beam wherein the first filtered beam is propagating in a direction opposite and substantially non-parallel to the first collimated beam and the second filtered beam is propagating in direction opposite and substantially parallel to said first collimated beam and provides optical feedback to said laser diode pump,

a mirror positioned adjacent to said laser diode pump whose reflective facet is placed at the focal plane of said first lens assembly and which receives and reflects said first filtered beam to produce a second collimated beam after collimation from said lens assembly, wherein second collimate beam produces said second filtered beam upon diffraction from said volume holographic grating element,

a second lens assembly to form a beam expander with first lens assembly for the second harmonic light.

37. The tunable laser of claim 36, wherein the laser pump diode is a single spatial mode semi-conductor laser diode.

38. The tunable laser of claim 36, wherein the laser pump diode is a broad area semi-conductor laser diode.

39. The tunable laser of claim 36, wherein the pump diode is an array of broad area semi-conductor laser diode.

40. The tunable laser of claim 36, wherein the reflective volume holographic grating element is made of photosensitive glass.

41. The tunable laser of claim 36, wherein the reflective volume holographic grating element contains one of more overlapped reflective gratings each with distinct grating vector.