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Photoconductive and photovoltaic metal-semiconductor-metal κ-Ga 2 O 3 solar-blind detectors with high rejection ratios
The metal-semiconductor-metal (MSM) structure is a popular architecture for developing Ga 2 O 3 solar blind photodetectors. The nature of metal-semiconductor contact is decisive for the operation mode, gain mechanism and device performances. In this contribution, κ -Ga 2 O 3 MSM solar-blind photodet...
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Published in: | Journal of physics. D, Applied physics Applied physics, 2022-09, Vol.55 (39), p.394003 |
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container_issue | 39 |
container_start_page | 394003 |
container_title | Journal of physics. D, Applied physics |
container_volume | 55 |
creator | Cui, Mei Xu, Yang Sun, Xinyu Wang, Zhengpeng Gong, Hehe Chen, Xuanhu Hu, Tiancheng Zhang, Yijun Ren, Fang-fang Gu, Shulin Ye, Jiandong Zhang, Rong |
description | The metal-semiconductor-metal (MSM) structure is a popular architecture for developing Ga
2
O
3
solar blind photodetectors. The nature of metal-semiconductor contact is decisive for the operation mode, gain mechanism and device performances. In this contribution,
κ
-Ga
2
O
3
MSM solar-blind photodetectors with Ti/Ga
2
O
3
Ohmic and Ni/Ga
2
O
3
Schottky contacts were constructed on the high-quality Si-doped
κ
-Ga
2
O
3
epilayer grown by hydride vapor phase epitaxy. The Ti/
κ
-Ga
2
O
3
/Ti Ohmic MSM device is operated in a photoconductive mode, exhibiting a maximum responsivity of 322.5 A W
−1
and a high rejection ratio of over 10
5
, but with an undesirable sub-gap response and high dark current. In comparison, the Ni/Ga
2
O
3
/Ni photodiode with a back-to-back Schottky configuration is operated in a mixed photovoltaic and photoconductive mode, demonstrating a decent photoresponsivity of 0.37 A W
−1
, a maintained high rejection ratio of 1.16 × 10
5
, a detectivity of 3.51 × 10
13
Jones and the elimination of slow photoresponse from sub-gap states. The frequency-dependent photoresponse and transient photocurrent characteristics indicate that the persistent photoconductivity effect is responsible for the high gain achieved in the Ti/Ga
2
O
3
/Ti photoconductor, and the dominant slow transient decay component is a fingerprint of photoexcited carrier trapping and repopulation. The response speed is improved in the Ni/Ga
2
O
3
/Ni Schottky MSM device, whereas carrier transport across interdigitated fingers is affected by bulk traps, limiting the overall response-bandwidth merit. |
doi_str_mv | 10.1088/1361-6463/ac7f68 |
format | article |
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2
O
3
solar blind photodetectors. The nature of metal-semiconductor contact is decisive for the operation mode, gain mechanism and device performances. In this contribution,
κ
-Ga
2
O
3
MSM solar-blind photodetectors with Ti/Ga
2
O
3
Ohmic and Ni/Ga
2
O
3
Schottky contacts were constructed on the high-quality Si-doped
κ
-Ga
2
O
3
epilayer grown by hydride vapor phase epitaxy. The Ti/
κ
-Ga
2
O
3
/Ti Ohmic MSM device is operated in a photoconductive mode, exhibiting a maximum responsivity of 322.5 A W
−1
and a high rejection ratio of over 10
5
, but with an undesirable sub-gap response and high dark current. In comparison, the Ni/Ga
2
O
3
/Ni photodiode with a back-to-back Schottky configuration is operated in a mixed photovoltaic and photoconductive mode, demonstrating a decent photoresponsivity of 0.37 A W
−1
, a maintained high rejection ratio of 1.16 × 10
5
, a detectivity of 3.51 × 10
13
Jones and the elimination of slow photoresponse from sub-gap states. The frequency-dependent photoresponse and transient photocurrent characteristics indicate that the persistent photoconductivity effect is responsible for the high gain achieved in the Ti/Ga
2
O
3
/Ti photoconductor, and the dominant slow transient decay component is a fingerprint of photoexcited carrier trapping and repopulation. The response speed is improved in the Ni/Ga
2
O
3
/Ni Schottky MSM device, whereas carrier transport across interdigitated fingers is affected by bulk traps, limiting the overall response-bandwidth merit.</description><identifier>ISSN: 0022-3727</identifier><identifier>EISSN: 1361-6463</identifier><identifier>DOI: 10.1088/1361-6463/ac7f68</identifier><language>eng</language><ispartof>Journal of physics. D, Applied physics, 2022-09, Vol.55 (39), p.394003</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c888-4e0e3c74f82e9c49fc5b9e47211460a81c167c1ff628efaf38fbb835b228b6523</citedby><cites>FETCH-LOGICAL-c888-4e0e3c74f82e9c49fc5b9e47211460a81c167c1ff628efaf38fbb835b228b6523</cites><orcidid>0000-0002-3985-6768 ; 0000-0002-3328-6186</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Cui, Mei</creatorcontrib><creatorcontrib>Xu, Yang</creatorcontrib><creatorcontrib>Sun, Xinyu</creatorcontrib><creatorcontrib>Wang, Zhengpeng</creatorcontrib><creatorcontrib>Gong, Hehe</creatorcontrib><creatorcontrib>Chen, Xuanhu</creatorcontrib><creatorcontrib>Hu, Tiancheng</creatorcontrib><creatorcontrib>Zhang, Yijun</creatorcontrib><creatorcontrib>Ren, Fang-fang</creatorcontrib><creatorcontrib>Gu, Shulin</creatorcontrib><creatorcontrib>Ye, Jiandong</creatorcontrib><creatorcontrib>Zhang, Rong</creatorcontrib><title>Photoconductive and photovoltaic metal-semiconductor-metal κ-Ga 2 O 3 solar-blind detectors with high rejection ratios</title><title>Journal of physics. D, Applied physics</title><description>The metal-semiconductor-metal (MSM) structure is a popular architecture for developing Ga
2
O
3
solar blind photodetectors. The nature of metal-semiconductor contact is decisive for the operation mode, gain mechanism and device performances. In this contribution,
κ
-Ga
2
O
3
MSM solar-blind photodetectors with Ti/Ga
2
O
3
Ohmic and Ni/Ga
2
O
3
Schottky contacts were constructed on the high-quality Si-doped
κ
-Ga
2
O
3
epilayer grown by hydride vapor phase epitaxy. The Ti/
κ
-Ga
2
O
3
/Ti Ohmic MSM device is operated in a photoconductive mode, exhibiting a maximum responsivity of 322.5 A W
−1
and a high rejection ratio of over 10
5
, but with an undesirable sub-gap response and high dark current. In comparison, the Ni/Ga
2
O
3
/Ni photodiode with a back-to-back Schottky configuration is operated in a mixed photovoltaic and photoconductive mode, demonstrating a decent photoresponsivity of 0.37 A W
−1
, a maintained high rejection ratio of 1.16 × 10
5
, a detectivity of 3.51 × 10
13
Jones and the elimination of slow photoresponse from sub-gap states. The frequency-dependent photoresponse and transient photocurrent characteristics indicate that the persistent photoconductivity effect is responsible for the high gain achieved in the Ti/Ga
2
O
3
/Ti photoconductor, and the dominant slow transient decay component is a fingerprint of photoexcited carrier trapping and repopulation. The response speed is improved in the Ni/Ga
2
O
3
/Ni Schottky MSM device, whereas carrier transport across interdigitated fingers is affected by bulk traps, limiting the overall response-bandwidth merit.</description><issn>0022-3727</issn><issn>1361-6463</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNo9kE1OwzAUhC0EEqWwZ-kLmPoncV6XqIKCVKksuo8c55m4SuLKDq24GofgTDRtxWqkTzOz-Ah5FPxJcICZUFownWk1M7ZwGq7I5B9dkwnnUjJVyOKW3KW05ZznGsSEHD6aMAQb-vrLDn6P1PQ13Y1sH9rBeEs7HEzLEnb-0gqRnRj9_WFLQyVdU0VTaE1kVeuP8xoHHGuJHvzQ0MZ_NjTi9sh86Gk0x0j35MaZNuHDJadk8_qyWbyx1Xr5vnheMQsALEOOyhaZA4lzm82dzas5ZoUUItPcgLBCF1Y4pyWgM06BqypQeSUlVDqXakr4-dbGkFJEV-6i70z8LgUvR2_lKKkcJZVnb-oPEX9kDg</recordid><startdate>20220929</startdate><enddate>20220929</enddate><creator>Cui, Mei</creator><creator>Xu, Yang</creator><creator>Sun, Xinyu</creator><creator>Wang, Zhengpeng</creator><creator>Gong, Hehe</creator><creator>Chen, Xuanhu</creator><creator>Hu, Tiancheng</creator><creator>Zhang, Yijun</creator><creator>Ren, Fang-fang</creator><creator>Gu, Shulin</creator><creator>Ye, Jiandong</creator><creator>Zhang, Rong</creator><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-3985-6768</orcidid><orcidid>https://orcid.org/0000-0002-3328-6186</orcidid></search><sort><creationdate>20220929</creationdate><title>Photoconductive and photovoltaic metal-semiconductor-metal κ-Ga 2 O 3 solar-blind detectors with high rejection ratios</title><author>Cui, Mei ; Xu, Yang ; Sun, Xinyu ; Wang, Zhengpeng ; Gong, Hehe ; Chen, Xuanhu ; Hu, Tiancheng ; Zhang, Yijun ; Ren, Fang-fang ; Gu, Shulin ; Ye, Jiandong ; Zhang, Rong</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c888-4e0e3c74f82e9c49fc5b9e47211460a81c167c1ff628efaf38fbb835b228b6523</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Cui, Mei</creatorcontrib><creatorcontrib>Xu, Yang</creatorcontrib><creatorcontrib>Sun, Xinyu</creatorcontrib><creatorcontrib>Wang, Zhengpeng</creatorcontrib><creatorcontrib>Gong, Hehe</creatorcontrib><creatorcontrib>Chen, Xuanhu</creatorcontrib><creatorcontrib>Hu, Tiancheng</creatorcontrib><creatorcontrib>Zhang, Yijun</creatorcontrib><creatorcontrib>Ren, Fang-fang</creatorcontrib><creatorcontrib>Gu, Shulin</creatorcontrib><creatorcontrib>Ye, Jiandong</creatorcontrib><creatorcontrib>Zhang, Rong</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of physics. D, Applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Cui, Mei</au><au>Xu, Yang</au><au>Sun, Xinyu</au><au>Wang, Zhengpeng</au><au>Gong, Hehe</au><au>Chen, Xuanhu</au><au>Hu, Tiancheng</au><au>Zhang, Yijun</au><au>Ren, Fang-fang</au><au>Gu, Shulin</au><au>Ye, Jiandong</au><au>Zhang, Rong</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Photoconductive and photovoltaic metal-semiconductor-metal κ-Ga 2 O 3 solar-blind detectors with high rejection ratios</atitle><jtitle>Journal of physics. D, Applied physics</jtitle><date>2022-09-29</date><risdate>2022</risdate><volume>55</volume><issue>39</issue><spage>394003</spage><pages>394003-</pages><issn>0022-3727</issn><eissn>1361-6463</eissn><abstract>The metal-semiconductor-metal (MSM) structure is a popular architecture for developing Ga
2
O
3
solar blind photodetectors. The nature of metal-semiconductor contact is decisive for the operation mode, gain mechanism and device performances. In this contribution,
κ
-Ga
2
O
3
MSM solar-blind photodetectors with Ti/Ga
2
O
3
Ohmic and Ni/Ga
2
O
3
Schottky contacts were constructed on the high-quality Si-doped
κ
-Ga
2
O
3
epilayer grown by hydride vapor phase epitaxy. The Ti/
κ
-Ga
2
O
3
/Ti Ohmic MSM device is operated in a photoconductive mode, exhibiting a maximum responsivity of 322.5 A W
−1
and a high rejection ratio of over 10
5
, but with an undesirable sub-gap response and high dark current. In comparison, the Ni/Ga
2
O
3
/Ni photodiode with a back-to-back Schottky configuration is operated in a mixed photovoltaic and photoconductive mode, demonstrating a decent photoresponsivity of 0.37 A W
−1
, a maintained high rejection ratio of 1.16 × 10
5
, a detectivity of 3.51 × 10
13
Jones and the elimination of slow photoresponse from sub-gap states. The frequency-dependent photoresponse and transient photocurrent characteristics indicate that the persistent photoconductivity effect is responsible for the high gain achieved in the Ti/Ga
2
O
3
/Ti photoconductor, and the dominant slow transient decay component is a fingerprint of photoexcited carrier trapping and repopulation. The response speed is improved in the Ni/Ga
2
O
3
/Ni Schottky MSM device, whereas carrier transport across interdigitated fingers is affected by bulk traps, limiting the overall response-bandwidth merit.</abstract><doi>10.1088/1361-6463/ac7f68</doi><orcidid>https://orcid.org/0000-0002-3985-6768</orcidid><orcidid>https://orcid.org/0000-0002-3328-6186</orcidid></addata></record> |
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source | Institute of Physics:Jisc Collections:IOP Publishing Read and Publish 2024-2025 (Reading List) |
title | Photoconductive and photovoltaic metal-semiconductor-metal κ-Ga 2 O 3 solar-blind detectors with high rejection ratios |
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