{"title":"基于无机过氧化物的克雷奇曼构型氢探测器","authors":"Qihui Ye, Gang Song","doi":"10.1007/s10825-024-02171-8","DOIUrl":null,"url":null,"abstract":"<div><p>We theoretically investigate a hydrogen (H<span>\\(_2\\)</span>) detector in a plasmonic structure involving an inorganic perovskite. The structure is composed of a prism, a silver layer, a perovskite layer (CsPbBr<span>\\(_3\\)</span>), and a palladium layer (Pd). The palladium layer absorbs H<sub>2</sub>, which transforms it into a Pd-H layer. Due to the large difference in dielectric constants between Pd and Pd-H, the reflection versus the incident angle <span>\\(\\theta\\)</span> exhibits great differences (<span>\\(\\Delta R\\)</span>) between the structures with a Pd layer and with a Pd-H layer. Our calculation results show that the working wavelength has a substantial impact on <span>\\(\\Delta R\\)</span>. The working wavelength not only affects the dielectric constants of the materials in our structure, but also influences the skin depth of surface plasmon polaritons (SPPs) in the CsPbBr<span>\\(_3\\)</span> layer, which couple with the Pd or Pd-H layers. A long working wavelength provides a longer skin depth, which couples more energy of the SPPs with the Pd or Pd-H layers. With an increase in Ag layer thickness, the dissipation of our proposed structure reduces the maximum value of <span>\\(\\Delta R\\)</span>. According to our calculations, there is an optimal thickness of the CsPbBr<span>\\(_3\\)</span> layer for which the value of <span>\\(\\Delta R\\)</span> is the largest. The results show the competition between the coupling and the dissipation of the SPP intensity along the direction perpendicular to the layers in the CsPbBr<span>\\(_3\\)</span> layer. At certain conditions, <span>\\(\\Delta R\\)</span> reaches a value of 0.13, which is about 20% of the reflection value. The detector we designed demonstrates good performance, with many potential applications.</p></div>","PeriodicalId":620,"journal":{"name":"Journal of Computational Electronics","volume":"23 3","pages":"672 - 676"},"PeriodicalIF":2.2000,"publicationDate":"2024-06-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Hydrogen detector in Kretschmann configuration based on an inorganic perovskite\",\"authors\":\"Qihui Ye, Gang Song\",\"doi\":\"10.1007/s10825-024-02171-8\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>We theoretically investigate a hydrogen (H<span>\\\\(_2\\\\)</span>) detector in a plasmonic structure involving an inorganic perovskite. The structure is composed of a prism, a silver layer, a perovskite layer (CsPbBr<span>\\\\(_3\\\\)</span>), and a palladium layer (Pd). The palladium layer absorbs H<sub>2</sub>, which transforms it into a Pd-H layer. Due to the large difference in dielectric constants between Pd and Pd-H, the reflection versus the incident angle <span>\\\\(\\\\theta\\\\)</span> exhibits great differences (<span>\\\\(\\\\Delta R\\\\)</span>) between the structures with a Pd layer and with a Pd-H layer. Our calculation results show that the working wavelength has a substantial impact on <span>\\\\(\\\\Delta R\\\\)</span>. The working wavelength not only affects the dielectric constants of the materials in our structure, but also influences the skin depth of surface plasmon polaritons (SPPs) in the CsPbBr<span>\\\\(_3\\\\)</span> layer, which couple with the Pd or Pd-H layers. A long working wavelength provides a longer skin depth, which couples more energy of the SPPs with the Pd or Pd-H layers. With an increase in Ag layer thickness, the dissipation of our proposed structure reduces the maximum value of <span>\\\\(\\\\Delta R\\\\)</span>. According to our calculations, there is an optimal thickness of the CsPbBr<span>\\\\(_3\\\\)</span> layer for which the value of <span>\\\\(\\\\Delta R\\\\)</span> is the largest. The results show the competition between the coupling and the dissipation of the SPP intensity along the direction perpendicular to the layers in the CsPbBr<span>\\\\(_3\\\\)</span> layer. At certain conditions, <span>\\\\(\\\\Delta R\\\\)</span> reaches a value of 0.13, which is about 20% of the reflection value. The detector we designed demonstrates good performance, with many potential applications.</p></div>\",\"PeriodicalId\":620,\"journal\":{\"name\":\"Journal of Computational Electronics\",\"volume\":\"23 3\",\"pages\":\"672 - 676\"},\"PeriodicalIF\":2.2000,\"publicationDate\":\"2024-06-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Computational Electronics\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s10825-024-02171-8\",\"RegionNum\":4,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Computational Electronics","FirstCategoryId":"5","ListUrlMain":"https://link.springer.com/article/10.1007/s10825-024-02171-8","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
Hydrogen detector in Kretschmann configuration based on an inorganic perovskite
We theoretically investigate a hydrogen (H\(_2\)) detector in a plasmonic structure involving an inorganic perovskite. The structure is composed of a prism, a silver layer, a perovskite layer (CsPbBr\(_3\)), and a palladium layer (Pd). The palladium layer absorbs H2, which transforms it into a Pd-H layer. Due to the large difference in dielectric constants between Pd and Pd-H, the reflection versus the incident angle \(\theta\) exhibits great differences (\(\Delta R\)) between the structures with a Pd layer and with a Pd-H layer. Our calculation results show that the working wavelength has a substantial impact on \(\Delta R\). The working wavelength not only affects the dielectric constants of the materials in our structure, but also influences the skin depth of surface plasmon polaritons (SPPs) in the CsPbBr\(_3\) layer, which couple with the Pd or Pd-H layers. A long working wavelength provides a longer skin depth, which couples more energy of the SPPs with the Pd or Pd-H layers. With an increase in Ag layer thickness, the dissipation of our proposed structure reduces the maximum value of \(\Delta R\). According to our calculations, there is an optimal thickness of the CsPbBr\(_3\) layer for which the value of \(\Delta R\) is the largest. The results show the competition between the coupling and the dissipation of the SPP intensity along the direction perpendicular to the layers in the CsPbBr\(_3\) layer. At certain conditions, \(\Delta R\) reaches a value of 0.13, which is about 20% of the reflection value. The detector we designed demonstrates good performance, with many potential applications.
期刊介绍:
he Journal of Computational Electronics brings together research on all aspects of modeling and simulation of modern electronics. This includes optical, electronic, mechanical, and quantum mechanical aspects, as well as research on the underlying mathematical algorithms and computational details. The related areas of energy conversion/storage and of molecular and biological systems, in which the thrust is on the charge transport, electronic, mechanical, and optical properties, are also covered.
In particular, we encourage manuscripts dealing with device simulation; with optical and optoelectronic systems and photonics; with energy storage (e.g. batteries, fuel cells) and harvesting (e.g. photovoltaic), with simulation of circuits, VLSI layout, logic and architecture (based on, for example, CMOS devices, quantum-cellular automata, QBITs, or single-electron transistors); with electromagnetic simulations (such as microwave electronics and components); or with molecular and biological systems. However, in all these cases, the submitted manuscripts should explicitly address the electronic properties of the relevant systems, materials, or devices and/or present novel contributions to the physical models, computational strategies, or numerical algorithms.