Wide shoulder, high order mode filter for thick-silicon waveguides

• US 10,088,629 B2
• Filed: 05/05/2017
• Issued: 10/02/2018
• Est. Priority Date: 03/07/2014
• Status: Active Grant

• Current Assignee: Skorpios Technologies Inc.
• Original Assignee: Skorpios Technologies Inc.
• Inventors: Sodagar, Majid, Askari, Murtaza, Li, Guoliang
• Primary Examiner(s): Hollweg, Thomas A
• Assistant Examiner(s): Anderson, Guy
• Application Number:
  US15/588,128
• Publication Number:
  US 20170242192A1
• Time in Patent Office: 515 Days
• Field of Search: 385 14- 15, 385 27- 31, 385129-132
• CPC Class Codes: G02B 2006/12035 Materials
• CPC Class Codes: G02B 2006/12097 Ridge, rib or the like
• CPC Class Codes: G02B 2006/12109 Filter
• CPC Class Codes: G02B 5/20 Filters polarising elements G02B5/30
• CPC Class Codes: G02B 6/122 Basic optical elements, e.g. light-guiding paths
• CPC Class Codes: G02B 6/1228 Tapered waveguides, e.g. integrated spot-size transformers for coupling with fibres G02B6/305
• CPC Class Codes: G02B 6/14 Mode converters
• CPC Class Codes: G02B 6/262 Optical details of coupling light into, or out of, or between fibre ends, e.g. special fibre end shapes or associated optical elements
• CPC Class Codes: G02F 1/3501 Constructional details or arrangements of non-linear optical devices, e.g. shape of non-linear crystals
• CPC Class Codes: G02F 1/3509 Shape, e.g. shape of end face
• CPC Class Codes: G02F 1/365 in an optical waveguide structure G02F1/377, G02F1/395 take precedence

Abstract

An optical filter for attenuating higher-order modes in an optical waveguide includes a shoulder slab formed of a first material having a first index of refraction and disposed on a second material having a second index of refraction, the first index of refraction being higher than the second index of refraction. The shoulder slab defines a near end having a first width, an intermediate section, adjacent to the first end section, and a far end section, adjacent to the intermediate section and opposite the first end section along a direction of beam propagation. The optical filter also includes a waveguide ridge, formed of the first material and disposed atop the shoulder slab, that traverses the shoulder slab, and is configured to guide light of a fundamental mode along the direction of beam propagation from the near end section to the far end section.

Claims

1. A laser, comprising:

first and second reflectors arranged to form an optical cavity therebetween;

a gain chip within the optical cavity;

an optical filter that attenuates higher order optical modes, wherein the optical filter is within the optical cavity and is optically connected with the gain chip; and

one or more waveguides that optically connect the gain chip and the optical filter with the first and second reflectors such that the optical cavity resonates at a resonant wavelength to form the laser;

wherein the one or more waveguides are capable of supporting both a fundamental optical mode and one or more higher order optical modes at the resonant wavelength;

wherein the optical filter attenuates the higher order optical modes sufficiently that the laser operates as a single mode laser; and

wherein at least one of the waveguides comprises;

a waveguide shoulder portion, formed of an optical material, that extends along a light propagation direction, and

forms a waveguide shoulder width transverse to the light propagation direction; and

a waveguide ridge portion, formed of the optical material, that is disposed atop the waveguide shoulder portion,

extends along the light propagation direction, and

forms a waveguide ridge width, transverse to the light propagation direction, that is narrower than the waveguide shoulder width;

and wherein the optical filter comprises;

a filter shoulder portion, formed of the optical material, that

adjoins the waveguide shoulder portion of at least one of the waveguides,

extends along the light propagation direction, and

forms a filter shoulder width, transverse to the light propagation direction, that is wider than the waveguide shoulder width.

2. The laser of claim 1, wherein the filter shoulder width is at least twice the waveguide shoulder width.

3. The laser of claim 1, wherein the filter shoulder width is at least three times the waveguide shoulder width.

4. The laser of claim 1, wherein a height of the waveguide shoulder portion is equal to a height of the filter shoulder portion.

5. The laser of claim 1, wherein a combined height of the waveguide shoulder portion and the waveguide ridge portion is 0.5 μ

m or greater, and less than or equal to 2.0 μ

m.

6. The laser of claim 1, wherein the optical material comprises silicon.

7. The laser of claim 1, wherein the optical filter further comprises a filter ridge portion, formed of the optical material, that adjoins the waveguide ridge portion of the at least one of the waveguides, and extends along the light propagation direction.

8. The laser of claim 7, wherein the filter ridge portion forms a filter ridge width that is transverse to the light propagation direction and remains constant along the light propagation direction from a near end of the optical filter to a far end of the optical filter.

9. The laser of claim 7, wherein the filter ridge portion forms a filter ridge width that tapers adiabatically inward, along the light propagation direction, from a near end of the optical filter to a central region of the optical filter, and tapers adiabatically outward from the central region to a far end of the optical filter.

10. The laser of claim 7, wherein a height of the filter shoulder portion is equal to a height of the waveguide shoulder portion, and a height of the filter ridge portion is equal to a height of the waveguide ridge portion.

11. The laser of claim 7, wherein the filter shoulder portion is less than or equal to 100 microns long from a near end of the optical filter to a far end of the optical filter.

12. The laser of claim 9, wherein:

the filter shoulder portion is about 100 microns long from the near end to the far end of the optical filter;

the filter ridge tapers adiabatically inward, along the light propagation direction, for about 30 microns from the near end of the optical filter to the central region of the optical filter;

the central region is about 40 microns long along the light propagation direction;

and filter ridge tapers adiabatically outward, along the light propagation direction, for about 30 microns from the central region to the far end of the optical filter.

13. A laser, comprising:

first and second reflectors arranged to form an optical cavity therebetween;

a gain chip within the optical cavity;

an optical filter that attenuates one or more higher order transverse optical modes, wherein the optical filter is within the optical cavity and is optically connected with the gain chip; and

waveguides that optically connect the gain chip and the optical filter with the first and second reflectors such that the optical cavity resonates at a resonant wavelength to form the laser;

wherein first and second ones of the waveguides that optically connect directly with the optical filter comprise;

a shoulder slab, formed of a first material having a first index of refraction and disposed on a second material having a second index of refraction, the first index of refraction being higher than the second index of refraction, each of the first and second ones of the waveguides defining a waveguide shoulder width, and

a waveguide ridge, formed of the first material and disposed atop the shoulder slab,

wherein dimensions of the waveguide ridge and the shoulder slab of each of the first and second ones of the waveguides are sufficient to guide light of at least a fundamental mode and the higher order transverse optical modes of the resonant wavelength along a direction of beam propagation;

and wherein the optical filter comprises;

a filter shoulder slab that is;

formed of a portion of the first material that extends continuously from the shoulder slab of the first one of the waveguides at a first end of the optical filter, through the filter shoulder slab, and into the shoulder slab of the second one of the waveguides, at a second end of the optical filter;

the filter shoulder slab being disposed on the second material and defining a filter shoulder width that is at least twice the waveguide shoulder width, and

a filter waveguide ridge that is;

disposed atop the shoulder slab; and

formed of a portion of the first material that extends continuously from the waveguide ridge of the first one of the waveguides, along the direction of beam propagation into the filter waveguide ridge, through the second end of the optical filter and into the waveguide ridge of the second one of the waveguides.

14. The laser of claim 13, wherein the higher order transverse optical modes are not guided within the optical filter, such that the higher order transverse optical modes are attenuated within the optical filter.

15. The laser of claim 13, wherein:

a height of the filter shoulder slab is equal to a height of the shoulder slab;

a height of the filter waveguide ridge is equal to a height of the waveguide ridge; and

a combined height of the shoulder slab and the waveguide ridge is 0.5 μ

m or greater, and less than or equal to 2.0 μ

m.

16. The laser of claim 13, wherein the first material comprises silicon.

17. The laser of claim 13, wherein the filter waveguide ridge forms a filter ridge width, transverse to the direction of beam propagation, that remains constant along the direction of beam propagation from the first end of the optical filter to the second end of the optical filter.

18. The laser of claim 13, wherein the filter waveguide ridge forms a filter ridge width, transverse to the direction of beam propagation, that tapers adiabatically inward, along the direction of beam propagation, from the first end of the optical filter to a central region of the optical filter, and tapers adiabatically outward from the central region to the second end of the optical filter.

19. The laser of claim 18, wherein:

the filter shoulder slab is about 100 microns long from the first end to the second end of the optical filter;

the filter ridge tapers adiabatically inward, along the direction of beam propagation, for about 30 microns from the first end of the optical filter to the central region of the optical filter;

the central region is about 40 microns long along the direction of beam propagation;

and filter ridge tapers adiabatically outward, along the direction of beam propagation, for about 30 microns from the central region to the second end of the optical filter.