Ring-modulated laser
US-2016204578-A1 · Jul 14, 2016 · US
US10090632B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10090632-B2 |
| Application number | US-201415110429-A |
| Country | US |
| Kind code | B2 |
| Filing date | Feb 28, 2014 |
| Priority date | Feb 28, 2014 |
| Publication date | Oct 2, 2018 |
| Grant date | Oct 2, 2018 |
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An example device in accordance with an aspect of the present disclosure includes a ring waveguide and bus waveguide. The ring waveguide has a first coupled portion associated with a first modal index, and the bus waveguide includes a second coupled portion associated with a second modal index. The second coupled portion is evanescently coupleable to the first coupled portion. A laser outcoupling and associated lasing output of the device is variable based on varying a difference between the first modal index and the second modal index to vary coupling between the first coupled portion and the second coupled portion, without varying modal indices of non-coupled portions of the ring waveguide and bus waveguide.
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What is claimed is: 1. A device comprising: a ring waveguide having a first coupled portion associated with a first modal index; a bus waveguide having a second coupled portion, associated with a second modal index wherein the second coupled portion is evanescently coupleable to the first coupled portion; and a capacitor structure to apply electrical carriers to vary a difference between the first modal index and the second modal index, without varying modal indices of non-coupled portions of the ring waveguide and the bus waveguide; wherein a laser outcoupling and associated lasing output of the device is variable based on an evanescent coupling between the first coupled portion and the second coupled portion, without varying modal indices of non-coupled portions of the ring waveguide and bus waveguide. 2. The device of claim 1 , wherein the ring waveguide is to serve as a laser cavity based on resonance of the ring waveguide. 3. The device of claim 1 , further comprising an output waveguide coupled to the ring waveguide based on a third coupled portion of the ring waveguide; wherein the bus waveguide is to serve as a laser cavity based on resonance of the bus waveguide; wherein the ring waveguide is passive and is to couple lasing output from the bus waveguide to the output waveguide. 4. The device of claim 1 , wherein the bus waveguide is a conformal waveguide that is curved corresponding to the coupling with the ring waveguide. 5. The device of claim 1 , wherein the difference between the first modal index and the second modal index is achieved based on changing an index of a cladding of at least one of: the first coupled portion of the ring waveguide, and the second coupled portion of the bus waveguide. 6. The device of claim 1 , wherein the ring waveguide is coplanar with the bus waveguide. 7. The device of claim 1 , wherein the ring waveguide is non-coplanar with, and vertically displaced relative to, the bus waveguide. 8. The device of claim 1 , wherein the capacitor structure comprises a dielectric layer sandwiched by semiconductor layers of the device. 9. A system comprising: a ring waveguide having a first coupled portion associated with a first modal index; a bus waveguide having a second coupled portion, associated with a second modal index, wherein the second coupled portion is evanescently coupled to the first coupled portion; and a quantum well structure, disposed in at least one of the ring waveguide or the bus waveguide, to vary a difference between the first modal index and the second modal index based on an electro-optic effect, wherein a laser outcoupling and associated lasing output of the system varies based on varying the difference between the first modal index and the second modal index to vary coupling between the first coupled portion and the second coupled portion, without varying modal indices of non-coupled portions of the ring waveguide and bus waveguide. 10. The system of claim 9 , wherein the quantum well structure is disposed in the bus waveguide to vary the second modal index of the second coupled portion of the bus waveguide without varying the first modal index of the ring waveguide, to vary the difference between the first modal index and the second modal index. 11. The system of claim 9 , wherein the quantum well structure is disposed in the ring waveguide to vary the first modal index of the ring waveguide without varying the second modal index of the bus waveguide, to vary the difference between the first modal index and the second modal index. 12. A method, comprising: applying an optical signal to at least one of a ring waveguide and a bus waveguide; varying a difference between a first modal index associated with a first coupled portion of the ring waveguide, and a second modal index associated with a second coupled portion of the bus waveguide using a modulation actuator based on at least one of electrical tuning, mechanical tuning, acoustic tuning, and magnetic tuning, wherein the second coupled portion is evanescently coupled to the first coupled portion; and varying a laser outcoupling and associated lasing output based on varying the difference between the first modal index and the second modal index, without varying modal indices of non-coupled portions of the ring waveguide and bus waveguide. 13. The method of claim 12 , wherein the associated lasing output is based on the optical signal. 14. The method of claim 12 , wherein the varying the difference further comprises varying the first modal index of the ring waveguide without varying the second modal index of the bus waveguide. 15. The method of claim 12 , wherein the varying the difference further comprises varying the second modal index of the second coupled portion of the bus waveguide without varying the first modal index of the ring waveguide. 16. The method of claim 12 , wherein the difference between the first modal index and the second modal index is achieved based on changing an index of a cladding of at least one of: the first coupled portion of the ring waveguide, and the second coupled portion of the bus waveguide. 17. The system of claim 9 , wherein the electro-optic effect is at least one of a plasma dispersion effect, a Kerr effect, a Quantum-confined Stark effect, a Franz-Keldysh effect, or a Pockels effect.
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which comprises an additional resonator · CPC title
Ring lasers {(fibre ring lasers H01S3/06791)} · CPC title
Coupled cavities (H01S5/14 takes precedence) · CPC title
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