Surface passivation of random alloy AlGaAsSb avalanche photodiode
AlGaAsSb attracts significant interest for near‐infrared avalanche photodiodes (APD). The authors report a two‐order reduction in the dark current and a six‐time enhancement of gain in random alloy (RA) AlGaAsSb APD that is surface passivated by conformal coating of Al 2 O 3 via atomic layer deposit...
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Published in | Electronics letters Vol. 59; no. 18 |
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Main Authors | , , , , , , , |
Format | Journal Article |
Language | English |
Published |
Stevenage
John Wiley & Sons, Inc
01.09.2023
Wiley |
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Online Access | Get full text |
ISSN | 0013-5194 1350-911X |
DOI | 10.1049/ell2.12956 |
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Abstract | AlGaAsSb attracts significant interest for near‐infrared avalanche photodiodes (APD). The authors report a two‐order reduction in the dark current and a six‐time enhancement of gain in random alloy (RA) AlGaAsSb APD that is surface passivated by conformal coating of Al 2 O 3 via atomic layer deposition (ALD). The dark currents of the APDs with 400‐µm diameter (dry etched) at 90% breakdown voltage (0.9 V br ) are (5.5 ± 0.5) × 10 −5 A, (2.1 ± 0.4) × 10 −5 A, and (6.2 ± 0.8) × 10 −7 A for non‐passivated, Si 3 N 4 passivated, and Al 2 O 3 passivated devices, respectively. The dark current at a gain of 10 for the Al 2 O 3 passivated device is 1 × 10 −8 A which is comparable to the reported value for 100‐µm diameter mesa diodes passivated by SU‐8. Maximum gain values of 6, 12, and 35 were obtained for non‐passivated, Si 3 N 4 passivated, and Al 2 O 3 passivated devices, respectively. Moreover, punch‐through capacitance of 8 pF in a spectral response of 450 to 850 nm was obtained. Thus, Al 2 O 3 passivation can be the best solution for antimonide optoelectronic devices. |
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AbstractList | AlGaAsSb attracts significant interest for near‐infrared avalanche photodiodes (APD). The authors report a two‐order reduction in the dark current and a six‐time enhancement of gain in random alloy (RA) AlGaAsSb APD that is surface passivated by conformal coating of Al 2 O 3 via atomic layer deposition (ALD). The dark currents of the APDs with 400‐µm diameter (dry etched) at 90% breakdown voltage (0.9 V br ) are (5.5 ± 0.5) × 10 −5 A, (2.1 ± 0.4) × 10 −5 A, and (6.2 ± 0.8) × 10 −7 A for non‐passivated, Si 3 N 4 passivated, and Al 2 O 3 passivated devices, respectively. The dark current at a gain of 10 for the Al 2 O 3 passivated device is 1 × 10 −8 A which is comparable to the reported value for 100‐µm diameter mesa diodes passivated by SU‐8. Maximum gain values of 6, 12, and 35 were obtained for non‐passivated, Si 3 N 4 passivated, and Al 2 O 3 passivated devices, respectively. Moreover, punch‐through capacitance of 8 pF in a spectral response of 450 to 850 nm was obtained. Thus, Al 2 O 3 passivation can be the best solution for antimonide optoelectronic devices. AlGaAsSb attracts significant interest for near‐infrared avalanche photodiodes (APD). The authors report a two‐order reduction in the dark current and a six‐time enhancement of gain in random alloy (RA) AlGaAsSb APD that is surface passivated by conformal coating of Al2O3 via atomic layer deposition (ALD). The dark currents of the APDs with 400‐µm diameter (dry etched) at 90% breakdown voltage (0.9 Vbr) are (5.5 ± 0.5) × 10−5 A, (2.1 ± 0.4) × 10−5 A, and (6.2 ± 0.8) × 10−7 A for non‐passivated, Si3N4 passivated, and Al2O3 passivated devices, respectively. The dark current at a gain of 10 for the Al2O3 passivated device is 1 × 10−8 A which is comparable to the reported value for 100‐µm diameter mesa diodes passivated by SU‐8. Maximum gain values of 6, 12, and 35 were obtained for non‐passivated, Si3N4 passivated, and Al2O3 passivated devices, respectively. Moreover, punch‐through capacitance of 8 pF in a spectral response of 450 to 850 nm was obtained. Thus, Al2O3 passivation can be the best solution for antimonide optoelectronic devices. Abstract AlGaAsSb attracts significant interest for near‐infrared avalanche photodiodes (APD). The authors report a two‐order reduction in the dark current and a six‐time enhancement of gain in random alloy (RA) AlGaAsSb APD that is surface passivated by conformal coating of Al2O3 via atomic layer deposition (ALD). The dark currents of the APDs with 400‐µm diameter (dry etched) at 90% breakdown voltage (0.9 Vbr) are (5.5 ± 0.5) × 10−5 A, (2.1 ± 0.4) × 10−5 A, and (6.2 ± 0.8) × 10−7 A for non‐passivated, Si3N4 passivated, and Al2O3 passivated devices, respectively. The dark current at a gain of 10 for the Al2O3 passivated device is 1 × 10−8 A which is comparable to the reported value for 100‐µm diameter mesa diodes passivated by SU‐8. Maximum gain values of 6, 12, and 35 were obtained for non‐passivated, Si3N4 passivated, and Al2O3 passivated devices, respectively. Moreover, punch‐through capacitance of 8 pF in a spectral response of 450 to 850 nm was obtained. Thus, Al2O3 passivation can be the best solution for antimonide optoelectronic devices. |
Author | Wang, Tiancai You, Minghui Zhuang, Qiandong Peng, Hongling Zheng, Wanhua Srivastava, Vibha Cao, Peng Kesaria, Manoj |
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Snippet | AlGaAsSb attracts significant interest for near‐infrared avalanche photodiodes (APD). The authors report a two‐order reduction in the dark current and a... Abstract AlGaAsSb attracts significant interest for near‐infrared avalanche photodiodes (APD). The authors report a two‐order reduction in the dark current and... |
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SubjectTerms | Aluminum oxide Atomic layer epitaxy Avalanche diodes avalanche photodiodes Dark current Electric fields Molecular beam epitaxy Optoelectronic devices passivation Passivity Photodiodes Silicon nitride Spectral sensitivity |
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Title | Surface passivation of random alloy AlGaAsSb avalanche photodiode |
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