Mingxin Hu, Yanjun Duan, Shengren Li, Lin Yang, Wenxin Dong, Wei Dang, Zheng Zhang, Jiaqi Liu, Zhiqiang Li
{"title":"Molecular Engineering of Hole-Selective Layer of TexSe1–x for High-Performance Short-Wave Infrared Photodetectors","authors":"Mingxin Hu, Yanjun Duan, Shengren Li, Lin Yang, Wenxin Dong, Wei Dang, Zheng Zhang, Jiaqi Liu, Zhiqiang Li","doi":"10.1021/acsphotonics.4c01967","DOIUrl":null,"url":null,"abstract":"Short-wavelength infrared (SWIR) photodetectors are essential to human activities in military and civilian fields, including night vision, remote sensing, telecommunication, medical applications, safety monitoring, and mineral identification. Recently, the tellurium–selenium (Te<sub><i>x</i></sub>Se<sub>1–<i>x</i></sub>) alloy has demonstrated considerable potential in infrared photodetection. However, the photodetectors still suffer from poor device performance. Herein, we present an interfacial engineering strategy to enhance carrier transport in the Te<sub><i>x</i></sub>Se<sub>1–<i>x</i></sub> photodetector by utilizing a self-assembled monolayer (SAM) of [2-(3,6-dimethoxy-9<i>H</i>-carbazol-9-yl)ethyl]phosphonic acid (MeO-2PACz) as an interface layer between the Te<sub><i>x</i></sub>Se<sub>1–<i>x</i></sub> active layer and the poly[bis(4-phenyl)(2,4,6-trimethylphenyl)amine (PTAA) hole transport layer. Density functional theory calculations and in-depth XPS analysis illustrate the occurrence of charge transfer and the formation of P–Se bonds at the Te<sub><i>x</i></sub>Se<sub>1–<i>x</i></sub>/SAM interface. This interfacial engineering approach leads to a more homogeneous surface potential, an increased built-in voltage, improved energy band alignment, and superior photoelectronic characteristics. The self-powered Te<sub><i>x</i></sub>Se<sub>1–<i>x</i></sub> photodetector exhibits an external quantum efficiency (EQE) of 46% ± 1% at 980 nm and 19.7% ± 0.5% at 1320 nm. This makes the first demonstration of Te<sub><i>x</i></sub>Se<sub>1–<i>x</i></sub> photodiode achieving a high responsivity of 0.49 A W<sup>–1</sup>, along with a record total noise determined realistic detectivity <i></i><span style=\"color: inherit;\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mo stretchy=\"false\">(</mo><msubsup><mrow><mi>D</mi></mrow><mrow><mn>2</mn></mrow><mrow><mo>*</mo></mrow></msubsup><mo stretchy=\"false\">)</mo></math>' role=\"presentation\" style=\"position: relative;\" tabindex=\"0\"><nobr aria-hidden=\"true\"><span style=\"width: 2.162em; display: inline-block;\"><span style=\"display: inline-block; position: relative; width: 1.935em; height: 0px; font-size: 110%;\"><span style=\"position: absolute; clip: rect(1.651em, 1001.88em, 2.957em, -999.997em); top: -2.554em; left: 0em;\"><span><span style=\"font-family: STIXMathJax_Main;\">(</span><span><span style=\"display: inline-block; position: relative; width: 1.253em; height: 0px;\"><span style=\"position: absolute; clip: rect(3.185em, 1000.74em, 4.151em, -999.997em); top: -3.974em; left: 0em;\"><span><span style=\"font-family: STIXMathJax_Normal-italic;\">𝐷</span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"position: absolute; clip: rect(3.469em, 1000.46em, 4.151em, -999.997em); top: -4.372em; left: 0.798em;\"><span><span style=\"font-size: 70.7%; font-family: STIXMathJax_Main;\">∗</span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span><span style=\"position: absolute; clip: rect(3.355em, 1000.46em, 4.151em, -999.997em); top: -3.747em; left: 0.798em;\"><span><span style=\"font-size: 70.7%; font-family: STIXMathJax_Main;\">2</span></span><span style=\"display: inline-block; width: 0px; height: 3.98em;\"></span></span></span></span><span style=\"font-family: STIXMathJax_Main;\">)</span></span><span style=\"display: inline-block; width: 0px; height: 2.56em;\"></span></span></span><span style=\"display: inline-block; overflow: hidden; vertical-align: -0.309em; border-left: 0px solid; width: 0px; height: 1.191em;\"></span></span></nobr><span role=\"presentation\"><math display=\"inline\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><mo stretchy=\"false\">(</mo><msubsup><mrow><mi>D</mi></mrow><mrow><mn>2</mn></mrow><mrow><mo>*</mo></mrow></msubsup><mo stretchy=\"false\">)</mo></math></span></span><script type=\"math/mml\"><math display=\"inline\"><mo stretchy=\"false\">(</mo><msubsup><mrow><mi>D</mi></mrow><mrow><mn>2</mn></mrow><mrow><mo>*</mo></mrow></msubsup><mo stretchy=\"false\">)</mo></math></script> of 7.69 × 10<sup>10</sup> Jones (and 5.75 × 10<sup>11</sup> Jones when considering only shot noise) at 1319 nm, combined with an ultrafast response time of <547 ns (as measured under femtosecond pulsed laser illumination). Moreover, the photocurrent of this photodetector remains almost unchanged even after 30 days of storage.","PeriodicalId":23,"journal":{"name":"ACS Photonics","volume":"10 213 1","pages":""},"PeriodicalIF":6.5000,"publicationDate":"2025-01-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Photonics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1021/acsphotonics.4c01967","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
Short-wavelength infrared (SWIR) photodetectors are essential to human activities in military and civilian fields, including night vision, remote sensing, telecommunication, medical applications, safety monitoring, and mineral identification. Recently, the tellurium–selenium (TexSe1–x) alloy has demonstrated considerable potential in infrared photodetection. However, the photodetectors still suffer from poor device performance. Herein, we present an interfacial engineering strategy to enhance carrier transport in the TexSe1–x photodetector by utilizing a self-assembled monolayer (SAM) of [2-(3,6-dimethoxy-9H-carbazol-9-yl)ethyl]phosphonic acid (MeO-2PACz) as an interface layer between the TexSe1–x active layer and the poly[bis(4-phenyl)(2,4,6-trimethylphenyl)amine (PTAA) hole transport layer. Density functional theory calculations and in-depth XPS analysis illustrate the occurrence of charge transfer and the formation of P–Se bonds at the TexSe1–x/SAM interface. This interfacial engineering approach leads to a more homogeneous surface potential, an increased built-in voltage, improved energy band alignment, and superior photoelectronic characteristics. The self-powered TexSe1–x photodetector exhibits an external quantum efficiency (EQE) of 46% ± 1% at 980 nm and 19.7% ± 0.5% at 1320 nm. This makes the first demonstration of TexSe1–x photodiode achieving a high responsivity of 0.49 A W–1, along with a record total noise determined realistic detectivity (𝐷∗2) of 7.69 × 1010 Jones (and 5.75 × 1011 Jones when considering only shot noise) at 1319 nm, combined with an ultrafast response time of <547 ns (as measured under femtosecond pulsed laser illumination). Moreover, the photocurrent of this photodetector remains almost unchanged even after 30 days of storage.
期刊介绍:
Published as soon as accepted and summarized in monthly issues, ACS Photonics will publish Research Articles, Letters, Perspectives, and Reviews, to encompass the full scope of published research in this field.