Effects of the intrinsic layer width on the band-to-band tunneling current in p-i-n GaN-based avalanche photodiodes
Source abstract
Abstract
Dark current is critical for GaN-based avalanche photodiodes because it significantly increases the noise current and limits the multiplication factor. It has been found that the band-to-band tunneling current is the dominant origin of the dark current for avalanche photodiodes at the onset of breakdown voltage. Experimentally, for GaN-based avalanche photodiodes with a thinner intrinsic layer, the dark current increases nearly exponentially with the applied voltage even at a lower bias voltage. In this paper, the intrinsic layer (i-layer) width of GaN-based avalanche photodiodes has been varied to study its effect on the band-to-band tunneling current. A widely used equation was used to calculate the band-to-band tunneling current of avalanche photodiodes with different i-layer widths (i-layer 0.1 µm, 0.2 µm and 0.4 µm). At −40 V, the band-to-band tunneling current significantly reduces by a magnitude of 10−15 A with an increase in the i-layer width from 0.1 µm to 0.2 µm, and a magnitude of 10−29 A with an increase in the i-layer width from 0.2 µm to 0.4 µm. Then, GaN-based avalanche photodiodes (i-layer 0.1 µm, 0.2 µm and 0.4 µm) with different-sized mesa were fabricated. Also, the measurement of dark current of all three different structures was performed, and their multiplication factors were given.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: GaN-based semiconductor devices and materials · Ga2O3 and related materials · Semiconductor Quantum Structures and Devices
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (21)
Show source-provided references
1. 10.1063/1.277219910.1063/1.2772199 ↗
2. 10.1016/j.photonics.2007.05.00110.1016/j.photonics.2007.05.001 ↗
3. 10.1063/1.183553710.1063/1.1835537 ↗
4. 10.1063/1.36267710.1063/1.362677 ↗
5. 10.1063/1.164402910.1063/1.1644029 ↗
6. 10.1063/1.148121110.1063/1.1481211 ↗
7. 10.1063/1.219162010.1063/1.2191620 ↗
8. 10.1063/1.186149810.1063/1.1861498 ↗
9. 10.1116/1.57621510.1116/1.576215 ↗
10. Moll J L · Physics of Semiconductors · 1964
11. 10.1049/el:1980054710.1049/el:19800547 ↗
12. 10.1063/1.9108910.1063/1.91089 ↗
13. 10.1109/JQE.1981.107105710.1109/JQE.1981.1071057 ↗
14. Xiangyi D Guo · 2005
15. 10.1063/1.185349810.1063/1.1853498 ↗
16. 10.1063/1.272071210.1063/1.2720712 ↗
17. 10.1063/1.235820710.1063/1.2358207 ↗
18. 10.1063/1.12563110.1063/1.125631 ↗
19. 10.1063/1.36421310.1063/1.364213 ↗
20. 10.1063/1.295200310.1063/1.2952003 ↗
21. 10.1109/JQE.2007.89790010.1109/JQE.2007.897900 ↗