S. Vahid Hosseini, Mohaddeseh Abbasnejad and Mohammad Reza Mohammadizadeh
{"title":"二氧化锡-1 的光学和热电特性理论分析","authors":"S. Vahid Hosseini, Mohaddeseh Abbasnejad and Mohammad Reza Mohammadizadeh","doi":"10.1039/D4TC02505A","DOIUrl":null,"url":null,"abstract":"<p >This study investigates the optical and thermoelectric properties of metallic (cubic TiO, monoclinic TiO, and γ-Ti<small><sub>3</sub></small>O<small><sub>5</sub></small>) and semiconducting (Ti<small><sub>2</sub></small>O<small><sub>3</sub></small>, α-Ti<small><sub>3</sub></small>O<small><sub>5</sub></small>, β-Ti<small><sub>3</sub></small>O<small><sub>5</sub></small>, Ti<small><sub>4</sub></small>O<small><sub>7</sub></small>, and Ti<small><sub>5</sub></small>O<small><sub>9</sub></small>) phases of Ti<small><sub><em>n</em></sub></small>O<small><sub>2<em>n</em>−1</sub></small>, using various functionals including PBE, mBJ, PBE+<em>U</em>, and YS-PBE0. The YS-PBE0 and random phase approximation approaches accurately predict the electronic and optical bandgaps for semiconducting phases, which align well with the experimental data. For the case of semiconducting phases, two significant optical absorption peaks are identified: one in the infrared due to (t<small><sub>2g</sub></small>–e<small><sub>g</sub></small>) interband transitions and another in the ultraviolet due to O-2p to Ti-3d intraband transitions. The semiconducting phases demonstrate impressive Seebeck coefficients (800–1200 μV K<small><sup>−1</sup></small>), driven by large effective mass and flat bands near the Fermi level. The electronic relaxation times are estimated to be 10<small><sup>−14</sup></small> to 10<small><sup>−16</sup></small> seconds for Ti<small><sub><em>n</em></sub></small>O<small><sub>2<em>n</em>−1</sub></small> structures. Although the thermoelectric figure of merit of Ti<small><sub><em>n</em></sub></small>O<small><sub>2<em>n</em>−1</sub></small> phases is low (<1), there is possibility for improvement through optimizing carrier concentration. These findings suggest that Ti<small><sub><em>n</em></sub></small>O<small><sub>2<em>n</em>−1</sub></small> can be considered as potential materials for thermoelectric applications.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":null,"pages":null},"PeriodicalIF":5.7000,"publicationDate":"2024-09-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Theoretical analysis of optical and thermoelectric characteristics of TinO2n−1†\",\"authors\":\"S. Vahid Hosseini, Mohaddeseh Abbasnejad and Mohammad Reza Mohammadizadeh\",\"doi\":\"10.1039/D4TC02505A\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >This study investigates the optical and thermoelectric properties of metallic (cubic TiO, monoclinic TiO, and γ-Ti<small><sub>3</sub></small>O<small><sub>5</sub></small>) and semiconducting (Ti<small><sub>2</sub></small>O<small><sub>3</sub></small>, α-Ti<small><sub>3</sub></small>O<small><sub>5</sub></small>, β-Ti<small><sub>3</sub></small>O<small><sub>5</sub></small>, Ti<small><sub>4</sub></small>O<small><sub>7</sub></small>, and Ti<small><sub>5</sub></small>O<small><sub>9</sub></small>) phases of Ti<small><sub><em>n</em></sub></small>O<small><sub>2<em>n</em>−1</sub></small>, using various functionals including PBE, mBJ, PBE+<em>U</em>, and YS-PBE0. The YS-PBE0 and random phase approximation approaches accurately predict the electronic and optical bandgaps for semiconducting phases, which align well with the experimental data. For the case of semiconducting phases, two significant optical absorption peaks are identified: one in the infrared due to (t<small><sub>2g</sub></small>–e<small><sub>g</sub></small>) interband transitions and another in the ultraviolet due to O-2p to Ti-3d intraband transitions. The semiconducting phases demonstrate impressive Seebeck coefficients (800–1200 μV K<small><sup>−1</sup></small>), driven by large effective mass and flat bands near the Fermi level. The electronic relaxation times are estimated to be 10<small><sup>−14</sup></small> to 10<small><sup>−16</sup></small> seconds for Ti<small><sub><em>n</em></sub></small>O<small><sub>2<em>n</em>−1</sub></small> structures. Although the thermoelectric figure of merit of Ti<small><sub><em>n</em></sub></small>O<small><sub>2<em>n</em>−1</sub></small> phases is low (<1), there is possibility for improvement through optimizing carrier concentration. These findings suggest that Ti<small><sub><em>n</em></sub></small>O<small><sub>2<em>n</em>−1</sub></small> can be considered as potential materials for thermoelectric applications.</p>\",\"PeriodicalId\":84,\"journal\":{\"name\":\"Journal of Materials Chemistry C\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":5.7000,\"publicationDate\":\"2024-09-14\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Materials Chemistry C\",\"FirstCategoryId\":\"1\",\"ListUrlMain\":\"https://pubs.rsc.org/en/content/articlelanding/2024/tc/d4tc02505a\",\"RegionNum\":2,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATERIALS SCIENCE, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Materials Chemistry C","FirstCategoryId":"1","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2024/tc/d4tc02505a","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
Theoretical analysis of optical and thermoelectric characteristics of TinO2n−1†
This study investigates the optical and thermoelectric properties of metallic (cubic TiO, monoclinic TiO, and γ-Ti3O5) and semiconducting (Ti2O3, α-Ti3O5, β-Ti3O5, Ti4O7, and Ti5O9) phases of TinO2n−1, using various functionals including PBE, mBJ, PBE+U, and YS-PBE0. The YS-PBE0 and random phase approximation approaches accurately predict the electronic and optical bandgaps for semiconducting phases, which align well with the experimental data. For the case of semiconducting phases, two significant optical absorption peaks are identified: one in the infrared due to (t2g–eg) interband transitions and another in the ultraviolet due to O-2p to Ti-3d intraband transitions. The semiconducting phases demonstrate impressive Seebeck coefficients (800–1200 μV K−1), driven by large effective mass and flat bands near the Fermi level. The electronic relaxation times are estimated to be 10−14 to 10−16 seconds for TinO2n−1 structures. Although the thermoelectric figure of merit of TinO2n−1 phases is low (<1), there is possibility for improvement through optimizing carrier concentration. These findings suggest that TinO2n−1 can be considered as potential materials for thermoelectric applications.
期刊介绍:
The Journal of Materials Chemistry is divided into three distinct sections, A, B, and C, each catering to specific applications of the materials under study:
Journal of Materials Chemistry A focuses primarily on materials intended for applications in energy and sustainability.
Journal of Materials Chemistry B specializes in materials designed for applications in biology and medicine.
Journal of Materials Chemistry C is dedicated to materials suitable for applications in optical, magnetic, and electronic devices.
Example topic areas within the scope of Journal of Materials Chemistry C are listed below. This list is neither exhaustive nor exclusive.
Bioelectronics
Conductors
Detectors
Dielectrics
Displays
Ferroelectrics
Lasers
LEDs
Lighting
Liquid crystals
Memory
Metamaterials
Multiferroics
Photonics
Photovoltaics
Semiconductors
Sensors
Single molecule conductors
Spintronics
Superconductors
Thermoelectrics
Topological insulators
Transistors