T. Dedova , R. Krautmann , M. Rusu , A. Katerski , M. Krunks , T. Unold , N. Spalatu , A. Mere , J. Sydorenko , M. Sibiński , I. Oja Acik
{"title":"采用 ALD 和 USP 方法合成的带有 TiO2 电子传输层的 Sb2S3 太阳能电池","authors":"T. Dedova , R. Krautmann , M. Rusu , A. Katerski , M. Krunks , T. Unold , N. Spalatu , A. Mere , J. Sydorenko , M. Sibiński , I. Oja Acik","doi":"10.1016/j.solmat.2024.113279","DOIUrl":null,"url":null,"abstract":"<div><div>Electronic characteristics were investigated for solar cells (SCs) based on FTO/TiO<sub>2</sub>/Sb<sub>2</sub>S<sub>3</sub>/P3HT/Au structure, employing TiO<sub>2</sub> electron transport layers (ETLs) fabricated by two different methods: ultrasonic spray pyrolysis (USP) and atomic layer deposition (ALD). Regardless of the deposition method, both ALD and USP-TiO<sub>2</sub> exhibit the anatase crystal structure. The calculated crystallite sizes, derived from the (101) reflection of TiO<sub>2</sub> layers using the Scherrer equation, show minimal variance between the two methods, with values 25 nm for USP and 30 nm for ALD TiO<sub>2</sub>, respectively. Optical band gaps (E<sub>g</sub>) were found to be 3.31 eV and 3.35 eV for USP and ALD methods, respectively. Exploring the thickness series of ALD-TiO<sub>2</sub>, ranging from 100 to 1000 cycles (approximately 5–75 nm), solar cell performance was evaluated, with the highest power conversion efficiency (PCE) of 3.3 % achieved using ALD-TiO<sub>2</sub> of 400 cycles (approximately 30 nm thick). Notably, SCs featuring USP TiO<sub>2</sub> ETL layers, with a thickness of approximately 35–40 nm, outperform their ALD-TiO<sub>2</sub> counterparts, improving PCE by 15 %, recording 4.0 % versus 3.3 %, respectively. This superiority in PCE is attributed to the more favorable conduction band minimum (CBM) position of USP-TiO<sub>2</sub> relative to the Fermi level, as revealed in the band diagram. Specifically, a lower CBM spike at the USP-TiO<sub>2</sub>/-Sb<sub>2</sub>S<sub>3</sub> interface indicates reduced recombination rates compared to those at the ALD-TiO<sub>2</sub>/-Sb<sub>2</sub>S<sub>3</sub> interface. This study offers valuable insights into enhancing SC performance by optimizing deposition methods and synthesis parameters of ETL layers.</div></div>","PeriodicalId":429,"journal":{"name":"Solar Energy Materials and Solar Cells","volume":"280 ","pages":"Article 113279"},"PeriodicalIF":6.3000,"publicationDate":"2024-11-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Sb2S3 solar cells with TiO2 electron transporting layers synthesized by ALD and USP methods\",\"authors\":\"T. Dedova , R. Krautmann , M. Rusu , A. Katerski , M. Krunks , T. Unold , N. Spalatu , A. Mere , J. Sydorenko , M. Sibiński , I. Oja Acik\",\"doi\":\"10.1016/j.solmat.2024.113279\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>Electronic characteristics were investigated for solar cells (SCs) based on FTO/TiO<sub>2</sub>/Sb<sub>2</sub>S<sub>3</sub>/P3HT/Au structure, employing TiO<sub>2</sub> electron transport layers (ETLs) fabricated by two different methods: ultrasonic spray pyrolysis (USP) and atomic layer deposition (ALD). Regardless of the deposition method, both ALD and USP-TiO<sub>2</sub> exhibit the anatase crystal structure. The calculated crystallite sizes, derived from the (101) reflection of TiO<sub>2</sub> layers using the Scherrer equation, show minimal variance between the two methods, with values 25 nm for USP and 30 nm for ALD TiO<sub>2</sub>, respectively. Optical band gaps (E<sub>g</sub>) were found to be 3.31 eV and 3.35 eV for USP and ALD methods, respectively. Exploring the thickness series of ALD-TiO<sub>2</sub>, ranging from 100 to 1000 cycles (approximately 5–75 nm), solar cell performance was evaluated, with the highest power conversion efficiency (PCE) of 3.3 % achieved using ALD-TiO<sub>2</sub> of 400 cycles (approximately 30 nm thick). Notably, SCs featuring USP TiO<sub>2</sub> ETL layers, with a thickness of approximately 35–40 nm, outperform their ALD-TiO<sub>2</sub> counterparts, improving PCE by 15 %, recording 4.0 % versus 3.3 %, respectively. This superiority in PCE is attributed to the more favorable conduction band minimum (CBM) position of USP-TiO<sub>2</sub> relative to the Fermi level, as revealed in the band diagram. Specifically, a lower CBM spike at the USP-TiO<sub>2</sub>/-Sb<sub>2</sub>S<sub>3</sub> interface indicates reduced recombination rates compared to those at the ALD-TiO<sub>2</sub>/-Sb<sub>2</sub>S<sub>3</sub> interface. This study offers valuable insights into enhancing SC performance by optimizing deposition methods and synthesis parameters of ETL layers.</div></div>\",\"PeriodicalId\":429,\"journal\":{\"name\":\"Solar Energy Materials and Solar Cells\",\"volume\":\"280 \",\"pages\":\"Article 113279\"},\"PeriodicalIF\":6.3000,\"publicationDate\":\"2024-11-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Solar Energy Materials and Solar Cells\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0927024824005919\",\"RegionNum\":2,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"ENERGY & FUELS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Solar Energy Materials and Solar Cells","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0927024824005919","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENERGY & FUELS","Score":null,"Total":0}
Sb2S3 solar cells with TiO2 electron transporting layers synthesized by ALD and USP methods
Electronic characteristics were investigated for solar cells (SCs) based on FTO/TiO2/Sb2S3/P3HT/Au structure, employing TiO2 electron transport layers (ETLs) fabricated by two different methods: ultrasonic spray pyrolysis (USP) and atomic layer deposition (ALD). Regardless of the deposition method, both ALD and USP-TiO2 exhibit the anatase crystal structure. The calculated crystallite sizes, derived from the (101) reflection of TiO2 layers using the Scherrer equation, show minimal variance between the two methods, with values 25 nm for USP and 30 nm for ALD TiO2, respectively. Optical band gaps (Eg) were found to be 3.31 eV and 3.35 eV for USP and ALD methods, respectively. Exploring the thickness series of ALD-TiO2, ranging from 100 to 1000 cycles (approximately 5–75 nm), solar cell performance was evaluated, with the highest power conversion efficiency (PCE) of 3.3 % achieved using ALD-TiO2 of 400 cycles (approximately 30 nm thick). Notably, SCs featuring USP TiO2 ETL layers, with a thickness of approximately 35–40 nm, outperform their ALD-TiO2 counterparts, improving PCE by 15 %, recording 4.0 % versus 3.3 %, respectively. This superiority in PCE is attributed to the more favorable conduction band minimum (CBM) position of USP-TiO2 relative to the Fermi level, as revealed in the band diagram. Specifically, a lower CBM spike at the USP-TiO2/-Sb2S3 interface indicates reduced recombination rates compared to those at the ALD-TiO2/-Sb2S3 interface. This study offers valuable insights into enhancing SC performance by optimizing deposition methods and synthesis parameters of ETL layers.
期刊介绍:
Solar Energy Materials & Solar Cells is intended as a vehicle for the dissemination of research results on materials science and technology related to photovoltaic, photothermal and photoelectrochemical solar energy conversion. Materials science is taken in the broadest possible sense and encompasses physics, chemistry, optics, materials fabrication and analysis for all types of materials.