Laser on silicon made with 2d material gain medium
US-2017338621-A1 · Nov 23, 2017 · US
US9356427B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9356427-B2 |
| Application number | US-201414513477-A |
| Country | US |
| Kind code | B2 |
| Filing date | Oct 14, 2014 |
| Priority date | Mar 28, 2014 |
| Publication date | May 31, 2016 |
| Grant date | May 31, 2016 |
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A multi-wavelength surface plasmon laser that simultaneously emits surface plasmons having a large number of wavelengths and includes an active layer whose thickness changes with position, and a metal cavity whose length changes with position so that light of different wavelengths is emitted according to position. Surface plasmons are generated at the interface between a metal layer and a semiconductor layer in response to the light of different wavelengths. The surface plasmons having different wavelengths may be resonated in the metal cavity whose length changes with position and may be emitted to the outside.
Opening claim text (preview).
What is claimed is: 1. A surface plasmon laser comprising: a metal layer; a semiconductor layer that is disposed on an upper surface of the metal layer and includes an active layer whose thickness changes along a first direction which is parallel to the upper surface of the metal layer; and a first reflector and a second reflector that protrude from the upper surface of the metal layer, are extended from the upper surface of the metal layer, and are respectively disposed opposite a front and a back of the semiconductor layer, wherein the first reflector and the second reflector form a resonant cavity for surface plasmons generated at an interface between the metal layer and the semiconductor layer, and a length of a resonant cavity changes along the first direction. 2. The surface plasmon laser of claim 1 , wherein the length of the resonant cavity changes with the thickness change of the active layer along the first direction. 3. The surface plasmon laser of claim 1 , wherein the length of the resonant cavity is determined by an interval between the first reflector and the second reflector along a second direction which is perpendicular to the first direction, and wherein the interval between the first reflector and the second reflector changes along the first direction. 4. The surface plasmon laser of claim 1 , wherein the thickness of the active layer continuously changes along the first direction. 5. The surface plasmon laser of claim 1 , wherein the thickness of the active layer discretely changes in a plurality of step portions along the first direction. 6. The surface plasmon laser of claim 1 , wherein the active layer comprises a plurality of regions whose thicknesses are different from each other and are spaced apart from each other. 7. The surface plasmon laser of claim 6 , wherein each of the plurality of regions of the active layer has a plurality of quantum dots, a plurality of diameters of the quantum dots disposed in each respective region are substantially equal, and the diameters of the quantum dots disposed in each respective region are different from a plurality of diameters of quantum dots disposed in other regions of the regions. 8. The surface plasmon laser of claim 1 , wherein the thickness of the active layer and the length of the resonant cavity changes symmetrically. 9. The surface plasmon laser of claim 1 , wherein the semiconductor layer comprises: a first clad layer disposed on the metal layer; the active layer disposed on the first clad layer; and a second clad layer disposed on the active layer. 10. The surface plasmon laser of claim 9 , wherein at least a portion of the first clad layer is buried in the metal layer. 11. The surface plasmon laser of claim 9 , further comprising: an electrode layer disposed on the second clad layer, and an insulating layer disposed at least partially around the second clad layer to prevent the metal layer from electrically contacting the second clad layer. 12. The surface plasmon laser of claim 1 , wherein the length of the resonant cavity continuously changes along the first direction. 13. The surface plasmon laser of claim 12 , wherein the first reflector and the second reflector form a flat surface, and the first reflector and the second reflector are not parallel to each other so that an interval between the first reflector and the second reflector continuously changes. 14. The surface plasmon laser of claim 13 , wherein at least one of the first reflector and the second reflector is disposed in a slant toward the front or the back of the semiconductor layer. 15. The surface plasmon laser of claim 1 , wherein the length of the resonant cavity discretely changes in a plurality of step portions along the first direction. 16. The surface plasmon laser of claim 15 , wherein at least one of the first reflector and the second reflector has a plurality of bent step portions. 17. The surface plasmon laser of claim 1 , wherein at least one of the first reflector and the second reflector includes a plurality of vertical reflective films that are parallel to each other. 18. The surface plasmon laser of claim 1 , further comprising: a transparent cover layer covering the upper surface of the metal layer and the semiconductor layer. 19. An optoelectronic integrated circuit including a surface plasmon laser, wherein the surface plasmon laser comprises: a metal layer; a semiconductor layer that is disposed on an upper surface of the metal layer and includes an active layer whose thickness changes along a first direction which is parallel to the upper surface of the metal layer; and a first reflector and a second reflector that protrude from the upper surface of the metal layer, are extended from the upper surface of the metal layer, and are respectively disposed opposite a front and a back of the semiconductor layer, wherein the first reflector and the second reflector form a resonant cavity for surface plasmons generated at an interface between the metal layer and the semiconductor layer, and a length of a resonant cavity changes along the first direction.
characterised by special cladding layers, e.g. details on band-discontinuities · CPC title
Details on the cavity length · CPC title
characterised by the material · CPC title
in a single cavity · CPC title
External cavity lasers (H01S5/18 takes precedence; mode locking H01S5/065) · CPC title
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