Avalanche photodiode structure
US-2022140157-A1 · May 5, 2022 · US
US12140707B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-12140707-B2 |
| Application number | US-201917274914-A |
| Country | US |
| Kind code | B2 |
| Filing date | Sep 9, 2019 |
| Priority date | Sep 10, 2018 |
| Publication date | Nov 12, 2024 |
| Grant date | Nov 12, 2024 |
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A single photon avalanche diode (SPAD) device is presented. The SPAD device comprising: a Si-based avalanche layer formed over an n-type semiconductor contact layer; a p-type charge sheet layer formed in or on the avalanche layer, the p-type charge sheet layer having an in-plane width; a Ge-based absorber layer, formed over the charge sheet layer and/or the avalanche layer, and overlapping the charge sheet layer, the Ge-based absorber layer having an in-plane width; wherein, at least in one in-plane direction, the in-plane width of the Ge-based absorber layer is greater than the in-plane width of the p-type charge sheet layer.
Opening claim text (preview).
The invention claimed is: 1. A single photon avalanche diode (SPAD) device comprising: a Si-based avalanche layer formed over an n-type semiconductor contact layer; a p-type charge sheet layer formed in or on the avalanche layer, the p-type charge sheet layer having an in-plane width; a Ge-based absorber layer, formed over the charge sheet layer and/or the avalanche layer, and overlapping the charge sheet layer, the Ge-based absorber layer having an in-plane width; wherein, at least in one in-plane direction, the in-plane width of the Ge-based absorber layer is greater than the in-plane width of the p-type charge sheet layer. 2. A SPAD device according to claim 1 wherein in all in-plane directions, the in-plane width of the Ge-based absorber layer is greater than the in-plane width of the p-type charge sheet layer. 3. A SPAD device according to claim 1 , further comprising: a p-type semiconductor contact layer formed over the absorber layer, the p-type semiconductor contact layer having an in-plane width, wherein at least part of the p-type semiconductor contact layer is formed substantially in register with at least part of the p-type charge sheet layer, with the Ge-based absorber layer interposed between them. 4. A SPAD device according to claim 3 wherein, at least in one in-plane direction, the in-plane width of the Ge-based absorber layer is greater than the in-plane width of the p-type semiconductor contact layer. 5. A SPAD device according to claim 3 wherein, in all in-plane directions, the in-plane width of the Ge-based absorber layer is greater than the in-plane width of the p-type semiconductor contact layer. 6. A SPAD device according to claim 3 wherein, in all in-plane directions, the in-plane width of the Ge-based absorber layer is greater than the in-plane width of the p-type semiconductor contact layer and greater than the in-plane width of the p-type charge sheet layer. 7. A SPAD device according to claim 3 wherein the entire p-type semiconductor contact layer is formed substantially in register with at least part of the p-type charge sheet layer. 8. A SPAD device according to claim 3 wherein at least in one in-plane direction, the in-plane width of the p-type charge sheet layer is greater than the in-plane width of the p-type semiconductor contact layer, and wherein the Ge-based absorber layer has a sidewall in said in-plane direction and the charge sheet layer has a lateral edge in said in-plane direction, and either: (a) when the Ge-based absorber layer has a thickness of at least 1 μm, the distance in the in-plane direction between the lateral edge of the charge sheet layer and the sidewall of the Ge-based absorber layer is at least 1 μm greater than the thickness of the Ge-based absorber layer; or (b) when the Ge-based absorber layer has a thickness of less than 1 μm, the distance in the in-plane direction between the lateral edge of the charge sheet layer and the sidewall of the Ge-based absorber layer is at least 1.0 μm. 9. A SPAD device according to claim 8 wherein the distance in the in-plane direction between the lateral edge of the charge sheet layer and the sidewall of the Ge-based absorber layer is at least 5 μm. 10. A SPAD device according to claim 3 , wherein the p-type semiconductor contact layer has a lateral edge in said in-plane direction and the charge sheet layer has a lateral edge in said in-plane direction, and either: (c) when the width of the charge sheet is at least 25 μm, a distance in the in-plane direction between the lateral edge of the charge sheet layer and the lateral edge of the p-type semiconductor contact layer is at least 2 μm; or (d) when the width of the charge sheet is less than 25 μm, a distance in the in-plane direction between the lateral edge of the charge sheet layer and the lateral edge of the p-type semiconductor contact layer is at least 1 μm. 11. A SPAD device according to claim 1 wherein the charge sheet layer has a maximum doping concentration at a depth in the range 10-100 nm from the surface of the Si-based avalanche layer. 12. A SPAD array comprising at least a 1×2 arrangement of SPAD devices each according to claim 1 and formed on a common substrate. 13. A SPAD array according to claim 12 wherein the respective Ge-based absorber layers of adjacent SPAD devices are laterally isolated by: (i) etching of a continuous Ge-based absorber layer to at least the depth of the p-type charge sheet layer in order to form the respective Ge-based absorber layers of adjacent SPAD devices; or (ii) doping of a continuous Ge-based absorber layer to at least the depth of the p-type charge sheet layer in order to form the respective Ge-based absorber layers of adjacent SPAD devices; or (iii) selective area growth of the respective Ge-based absorber layers within patterned electrically insulating layers in order to form the respective Ge absorber layers of adjacent SPAD devices. 14. A LIDAR system comprising a source of light of wavelength in the range 0.9-2.0 μm and a SPAD device according to claim 1 . 15. Use of a SPAD device according to claim 1 in the detection of at least one photon with wavelength in the range 0.9-2.0 μm. 16. A method of manufacture of a SPAD device according to claim 1 wherein the p-type charge sheet layer is formed by selective area implantation into the Si-based avalanche layer. 17. A method according to claim 16 wherein the charge sheet layer is activated by annealing at a temperature of at least 850° C., before deposition of the Ge-based absorber layer. 18. A method according to claim 16 wherein at least one upper and/or side surface of the Ge-based absorber layer is passivated. 19. A method according to claim 18 wherein the passivation is provided by a GeO 2 layer thermally grown and protected by an Al 2 O 3 layer. 20. A single photon avalanche diode (SPAD) device comprising: a Si-based avalanche layer on an n-type semiconductor contact layer; a p-type charge sheet layer in or on the avalanche layer, the p-type charge sheet layer having an in-plane width; a Ge-based absorber layer, over the charge sheet layer and/or the avalanche layer, and overlapping the charge sheet layer, the Ge-based absorber layer having an in-plane width; and a p-type semiconductor contact layer over the Ge-based absorber layer, the p-type semiconductor contact layer having an in-plane width, wherein, at least in one in-plane direction, the in-plane width of the Ge-based absorber layer is greater than the in-plane width of the p-type charge sheet layer, and wherein, in all in-plane directions, the in-plane width of the Ge-based absorber layer is greater than the in-plane width of the p-type semiconductor contact layer.
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