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

• US 10,295,746 B2
• Filed: 08/28/2018
• Issued: 05/21/2019
• 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 G
• Application Number:
  US16/115,104
• Publication Number:
  US 20190094464A1
• Time in Patent Office: 266 Days
• 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. An optical filter for attenuating higher-order transverse modes, the optical filter comprising:

a shoulder slab, wherein;

the shoulder slab is formed of a first material having a first index of refraction and is disposed atop a second material having a second index of refraction, the first index of refraction being higher than the second index of refraction; and

a waveguide ridge disposed atop the shoulder slab, wherein;

the waveguide ridge is formed of the first material;

the waveguide ridge forms an input width in a first waveguide section along a direction of beam propagation, wherein;

a first filter section, formed by the shoulder slab and the waveguide ridge in the first waveguide section, is capable of guiding light of a fundamental mode and the higher-order transverse modes along the direction of beam propagation; and

the waveguide ridge tapers adiabatically inward from the input width to a reduced width, in a second waveguide section that adjoins the first waveguide section along the direction of beam propagation, wherein;

a second filter section, formed by the shoulder slab and the tapering waveguide ridge in the second waveguide section, is capable of guiding the fundamental mode, wherein the higher-order transverse modes are pushed into the shoulder slab where they are less strongly guided than the fundamental mode,

such that a proportion of energy guided in the fundamental mode, to energy guided in the higher-order transverse modes, increases along the direction of beam propagation in the second filter section.

2. The optical filter of claim 1, wherein:

the waveguide ridge remains constant in width at the reduced width, in a third filter section that adjoins the second filter section, along the direction of beam propagation.

3. The optical filter of claim 2, wherein:

the waveguide ridge tapers adiabatically outward from the reduced width to an output width, in a fourth filter section that adjoins the third filter section along the direction of beam propagation.

4. The optical filter of claim 1, wherein the direction of beam propagation defined by the waveguide ridge is a straight line at least through the first filter section and the second filter section.

5. The optical filter of claim 1, wherein a combined height of the shoulder slab and the waveguide ridge is greater than 0.5 μ

m and less than 2.0 μ

m.

6. The optical filter of claim 1, wherein the first material is crystalline silicon.

7. The optical filter claim 1, wherein a combined length of the first and second filter sections is less than or equal to 100 microns.

8. The optical filter of claim 1, further comprising:

an input waveguide, comprising an input shoulder slab and an input waveguide ridge, the input waveguide being optically coupled with the first filter section along the direction of beam propagation; and

an output waveguide, comprising an output shoulder slab and an output waveguide ridge, the output waveguide being optically coupled with the second filter section along the direction of beam propagation.

9. The optical filter of claim 8, wherein the shoulder slab of the optical filter is at least twice as wide, transverse to the direction of beam propagation, as the shoulder slab of the input waveguide.

10. The optical filter of claim 9, wherein the shoulder slab of the optical filter forms beveled corners.

11. The optical filter of claim 1, wherein the optical filter is symmetric along an axis running along the direction of beam propagation.

12. The optical filter of claim 1, further comprising:

reflectors that are operably coupled by waveguides to form an optical cavity, and

a light source that generates the light of the fundamental mode and the higher-order transverse modes, wherein;

the light source is operably coupled within the optical cavity to form a laser, and

the optical filter is operably coupled within the optical cavity such that the optical filter reduces the higher-order transverse modes in an output of the laser.

13. A method for filtering higher-order transverse modes in a ridge waveguide, the method comprising:

transmitting a beam of light, comprising a fundamental mode and one or more higher-order transverse modes, along a direction of beam propagation in a first ridge waveguide, wherein the first ridge waveguide includes;

a waveguide shoulder slab, formed of a first material disposed atop a substrate material, the first material having a higher index of refraction than the substrate material, and

a waveguide ridge, formed of the first material, disposed atop the waveguide shoulder slab and having an input waveguide ridge width, wherein a combination of the waveguide ridge and the waveguide shoulder slab is capable of guiding the fundamental mode and the one or more higher-order transverse modes;

coupling the beam of light along the direction of beam propagation into an optical filter, wherein the optical filter comprises;

a filter shoulder slab, formed of the first material and disposed atop the substrate material, and

a filter ridge, formed of the first material, disposed atop the filter shoulder slab and having a filter ridge width, wherein;

the filter ridge width matches the input waveguide ridge width where the beam of light couples from the first ridge waveguide into the optical filter, and

the filter ridge width decreases by adiabatically tapering along the direction of beam propagation such that the fundamental mode continues to be guided by the filter ridge, while at least a portion of the one or more higher-order transverse modes are pushed into the filter shoulder slab, attenuating the one or more higher-order transverse modes in the filter ridge; and

coupling the fundamental mode into a second ridge waveguide, after the fundamental mode has passed through the optical filter and the one or more higher-order transverse modes are attenuated in the filter ridge.

14. The method for filtering higher-order transverse modes of claim 13, wherein during the steps of transmitting the beam of light along the direction of beam propagation in the first ridge waveguide, coupling the beam of light along the direction of beam propagation into the optical filter, and coupling the light of the fundamental mode into the second ridge waveguide, the direction of beam propagation remains a straight line from the first ridge waveguide, through the optical filter and into the second ridge waveguide.

15. The method for filtering higher-order transverse modes of claim 13, wherein:

the filter ridge is a first filter ridge portion, and the filter ridge width is a first filter ridge width; and

coupling the beam of light along the direction of beam propagation into the optical filter comprises coupling the beam of light into a second filter ridge portion that has a constant second filter ridge width, the second filter ridge width matching the first filter ridge width after the first filter ridge width decreases by adiabatically tapering along the direction of beam propagation.

16. The method for filtering higher-order transverse modes of claim 15, further comprising coupling the beam of light along the direction of beam propagation from the second filter ridge portion into a third filter ridge portion that has a third filter ridge width, wherein:

the third filter ridge width increases by adiabatically tapering along the direction of beam propagation;

coupling the fundamental mode into the second ridge waveguide comprises coupling the fundamental mode from the third filter ridge portion into the second ridge waveguide; and

where the beam of light couples from the third filter ridge portion into the second ridge waveguide, the third filter ridge width matches a ridge width of the second ridge waveguide.

17. The method for filtering higher-order transverse modes of claim 13, wherein:

the waveguide shoulder slab has a waveguide shoulder slab width;

the filter shoulder slab has a filter shoulder slab width that is at least twice the waveguide shoulder slab width; and

coupling the beam of light along the direction of beam propagation into the optical filter comprises diffracting the higher-order transverse modes away from the direction of beam propagation.

18. The method for filtering higher-order transverse modes of claim 13, further comprising:

providing reflectors that are operably coupled through at least the first ridge waveguide and the second ridge waveguide to form an optical cavity therebetween;

operably coupling a source of light that generates the fundamental mode and the one or more higher-order transverse modes within the optical cavity so as to form a laser; and

operably coupling the optical filter within the optical cavity such that the optical filter reduces the higher-order transverse modes in an output of the laser.

19. An optical filter for reducing higher-order transverse modes in an output of a semiconductor laser, the optical filter comprising:

a shoulder slab, wherein;

the shoulder slab is formed of a first material having a first index of refraction and is disposed atop a second material having a second index of refraction, the first index of refraction being higher than the second index of refraction; and

a waveguide ridge disposed atop the shoulder slab, wherein;

the waveguide ridge is formed of the first material;

the waveguide ridge forms an input width in a first waveguide section along a direction of beam propagation, wherein;

a first filter section, formed by the shoulder slab and the waveguide ridge in the first waveguide section, is capable of guiding light of a fundamental mode and the higher-order transverse modes along the direction of beam propagation; and

the waveguide ridge tapers adiabatically inward from the input width to a reduced width, in a second waveguide section that adjoins the first waveguide section along the direction of beam propagation, wherein;

a second filter section, formed by the shoulder slab and the tapering waveguide ridge in the second waveguide section, is capable of guiding the fundamental mode, wherein the higher-order transverse modes are pushed into the shoulder slab where they are less strongly guided than the fundamental mode,

and wherein the optical filter is operably coupled within an optical cavity of the semiconductor laser, and increases a proportion of energy in the fundamental mode, to energy in the higher-order transverse modes, in the output of the laser.