Surface engineering of zinc oxide thin as an electron transport layer for perovskite solar cells

This work investigates the zinc oxide (ZnO) deposited by the spin coating technique which has for the main advantage of its implementation. Zinc oxide is a semiconductor that has a direct optical bandgap of 3.3 eV which has transparency properties of about 80% optical, anti-reflection in the UV-Vis...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Optical and quantum electronics 2023-07, Vol.55 (7), Article 574
Hauptverfasser: Koné, Klègayéré Emmanuel, Bouich, Amal, Soro, Donafologo, Soucase, Bernabé Marí
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page
container_issue 7
container_start_page
container_title Optical and quantum electronics
container_volume 55
creator Koné, Klègayéré Emmanuel
Bouich, Amal
Soro, Donafologo
Soucase, Bernabé Marí
description This work investigates the zinc oxide (ZnO) deposited by the spin coating technique which has for the main advantage of its implementation. Zinc oxide is a semiconductor that has a direct optical bandgap of 3.3 eV which has transparency properties of about 80% optical, anti-reflection in the UV-Vis spectrum, and high electrical conductivity (Cao et al. 2018). The electron transport layer (ETL) is one of its main functions in a solar cell. The number of spin coatings was changed from 1 to 4 in order to get different variations of ZnO thicknesses. These different samples were characterized. X-Ray Diffraction (XRD) showed the polycrystalline character of the ZnO films. Two peaks (the strongest) have been identified on planes (002) and (101). SEM showed that the surface of the samples presents a good crystallinity, which agrees with the results of XRD. Moreover, the crystallinity and the density increase with the number of cycles. The transmittance of samples obtained by spectrophotometry was about 80% in the visible and decreases with the number of cycles. Bandgap was calculated from absorbance data and it varies from 3.25 to 3.29 eV. The best sample was the sample with four cycles (ZnO-4). It was used for heterojunction with mixed halide methylammonium lead (MAPbBr 2 I). The bandgap obtained of the heterojunction MAPbBr 2 I/ZnO-4 was 1.9 eV. The simulation of the mixed halide methylammonium lead (MAPbBr 2 I) base-solar cell resulted in 16.938095 mA/cm 2 , 2 V, and 33.88% for Jsc, Voc, and eta respectively.
doi_str_mv 10.1007/s11082-023-04671-6
format Article
fullrecord <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_journals_2811673311</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2811673311</sourcerecordid><originalsourceid>FETCH-LOGICAL-c319t-f2b507da4715c7812fc2d4d494e906e04f9cb16bd7b785288a4453e5fb52ad9d3</originalsourceid><addsrcrecordid>eNp9kE1LxDAURYMoOI7-AVcB19G8NG3apYhfMOBCBXcxTV_GjjWpSUccf70dK7hzdTf33AuHkGPgp8C5OksAvBSMi4xxWShgxQ6ZQa4EK0E97ZIZz3jBygqqfXKQ0opzXsicz8jz_To6Y5GiX7YeMbZ-SYOjX623NHy2DdLhpfXUJGo8xQ7tEIOnQzQ-9SEOtDMbjNSFSHuM4SO9tgPSFDoTqcWuS4dkz5ku4dFvzsnj1eXDxQ1b3F3fXpwvmM2gGpgTdc5VY6SC3KoShLOikY2sJFa8QC5dZWso6kbVqsxFWRop8wxzV-fCNFWTzcnJtNvH8L7GNOhVWEc_XmpRAhQqywDGlphaNoaUIjrdx_bNxI0Grrcm9WRSjyb1j0ldjFA2Qanf6sH4N_0P9Q08X3dY</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2811673311</pqid></control><display><type>article</type><title>Surface engineering of zinc oxide thin as an electron transport layer for perovskite solar cells</title><source>SpringerLink</source><creator>Koné, Klègayéré Emmanuel ; Bouich, Amal ; Soro, Donafologo ; Soucase, Bernabé Marí</creator><creatorcontrib>Koné, Klègayéré Emmanuel ; Bouich, Amal ; Soro, Donafologo ; Soucase, Bernabé Marí</creatorcontrib><description>This work investigates the zinc oxide (ZnO) deposited by the spin coating technique which has for the main advantage of its implementation. Zinc oxide is a semiconductor that has a direct optical bandgap of 3.3 eV which has transparency properties of about 80% optical, anti-reflection in the UV-Vis spectrum, and high electrical conductivity (Cao et al. 2018). The electron transport layer (ETL) is one of its main functions in a solar cell. The number of spin coatings was changed from 1 to 4 in order to get different variations of ZnO thicknesses. These different samples were characterized. X-Ray Diffraction (XRD) showed the polycrystalline character of the ZnO films. Two peaks (the strongest) have been identified on planes (002) and (101). SEM showed that the surface of the samples presents a good crystallinity, which agrees with the results of XRD. Moreover, the crystallinity and the density increase with the number of cycles. The transmittance of samples obtained by spectrophotometry was about 80% in the visible and decreases with the number of cycles. Bandgap was calculated from absorbance data and it varies from 3.25 to 3.29 eV. The best sample was the sample with four cycles (ZnO-4). It was used for heterojunction with mixed halide methylammonium lead (MAPbBr 2 I). The bandgap obtained of the heterojunction MAPbBr 2 I/ZnO-4 was 1.9 eV. The simulation of the mixed halide methylammonium lead (MAPbBr 2 I) base-solar cell resulted in 16.938095 mA/cm 2 , 2 V, and 33.88% for Jsc, Voc, and eta respectively.</description><identifier>ISSN: 0306-8919</identifier><identifier>EISSN: 1572-817X</identifier><identifier>DOI: 10.1007/s11082-023-04671-6</identifier><language>eng</language><publisher>New York: Springer US</publisher><subject>Characterization and Evaluation of Materials ; Computer Communication Networks ; Crystallinity ; Electrical Engineering ; Electrical resistivity ; Electron transport ; Energy gap ; Heterojunctions ; Lasers ; Mathematical analysis ; Optical Devices ; Optical properties ; Optics ; Perovskites ; Photonics ; Photovoltaic cells ; Physics ; Physics and Astronomy ; Solar cells ; Spectrophotometry ; Spin coating ; Spin coatings ; X-ray diffraction ; Zinc oxide ; Zinc oxides</subject><ispartof>Optical and quantum electronics, 2023-07, Vol.55 (7), Article 574</ispartof><rights>The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c319t-f2b507da4715c7812fc2d4d494e906e04f9cb16bd7b785288a4453e5fb52ad9d3</citedby><cites>FETCH-LOGICAL-c319t-f2b507da4715c7812fc2d4d494e906e04f9cb16bd7b785288a4453e5fb52ad9d3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s11082-023-04671-6$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s11082-023-04671-6$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27922,27923,41486,42555,51317</link.rule.ids></links><search><creatorcontrib>Koné, Klègayéré Emmanuel</creatorcontrib><creatorcontrib>Bouich, Amal</creatorcontrib><creatorcontrib>Soro, Donafologo</creatorcontrib><creatorcontrib>Soucase, Bernabé Marí</creatorcontrib><title>Surface engineering of zinc oxide thin as an electron transport layer for perovskite solar cells</title><title>Optical and quantum electronics</title><addtitle>Opt Quant Electron</addtitle><description>This work investigates the zinc oxide (ZnO) deposited by the spin coating technique which has for the main advantage of its implementation. Zinc oxide is a semiconductor that has a direct optical bandgap of 3.3 eV which has transparency properties of about 80% optical, anti-reflection in the UV-Vis spectrum, and high electrical conductivity (Cao et al. 2018). The electron transport layer (ETL) is one of its main functions in a solar cell. The number of spin coatings was changed from 1 to 4 in order to get different variations of ZnO thicknesses. These different samples were characterized. X-Ray Diffraction (XRD) showed the polycrystalline character of the ZnO films. Two peaks (the strongest) have been identified on planes (002) and (101). SEM showed that the surface of the samples presents a good crystallinity, which agrees with the results of XRD. Moreover, the crystallinity and the density increase with the number of cycles. The transmittance of samples obtained by spectrophotometry was about 80% in the visible and decreases with the number of cycles. Bandgap was calculated from absorbance data and it varies from 3.25 to 3.29 eV. The best sample was the sample with four cycles (ZnO-4). It was used for heterojunction with mixed halide methylammonium lead (MAPbBr 2 I). The bandgap obtained of the heterojunction MAPbBr 2 I/ZnO-4 was 1.9 eV. The simulation of the mixed halide methylammonium lead (MAPbBr 2 I) base-solar cell resulted in 16.938095 mA/cm 2 , 2 V, and 33.88% for Jsc, Voc, and eta respectively.</description><subject>Characterization and Evaluation of Materials</subject><subject>Computer Communication Networks</subject><subject>Crystallinity</subject><subject>Electrical Engineering</subject><subject>Electrical resistivity</subject><subject>Electron transport</subject><subject>Energy gap</subject><subject>Heterojunctions</subject><subject>Lasers</subject><subject>Mathematical analysis</subject><subject>Optical Devices</subject><subject>Optical properties</subject><subject>Optics</subject><subject>Perovskites</subject><subject>Photonics</subject><subject>Photovoltaic cells</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Solar cells</subject><subject>Spectrophotometry</subject><subject>Spin coating</subject><subject>Spin coatings</subject><subject>X-ray diffraction</subject><subject>Zinc oxide</subject><subject>Zinc oxides</subject><issn>0306-8919</issn><issn>1572-817X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNp9kE1LxDAURYMoOI7-AVcB19G8NG3apYhfMOBCBXcxTV_GjjWpSUccf70dK7hzdTf33AuHkGPgp8C5OksAvBSMi4xxWShgxQ6ZQa4EK0E97ZIZz3jBygqqfXKQ0opzXsicz8jz_To6Y5GiX7YeMbZ-SYOjX623NHy2DdLhpfXUJGo8xQ7tEIOnQzQ-9SEOtDMbjNSFSHuM4SO9tgPSFDoTqcWuS4dkz5ku4dFvzsnj1eXDxQ1b3F3fXpwvmM2gGpgTdc5VY6SC3KoShLOikY2sJFa8QC5dZWso6kbVqsxFWRop8wxzV-fCNFWTzcnJtNvH8L7GNOhVWEc_XmpRAhQqywDGlphaNoaUIjrdx_bNxI0Grrcm9WRSjyb1j0ldjFA2Qanf6sH4N_0P9Q08X3dY</recordid><startdate>20230701</startdate><enddate>20230701</enddate><creator>Koné, Klègayéré Emmanuel</creator><creator>Bouich, Amal</creator><creator>Soro, Donafologo</creator><creator>Soucase, Bernabé Marí</creator><general>Springer US</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20230701</creationdate><title>Surface engineering of zinc oxide thin as an electron transport layer for perovskite solar cells</title><author>Koné, Klègayéré Emmanuel ; Bouich, Amal ; Soro, Donafologo ; Soucase, Bernabé Marí</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c319t-f2b507da4715c7812fc2d4d494e906e04f9cb16bd7b785288a4453e5fb52ad9d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Characterization and Evaluation of Materials</topic><topic>Computer Communication Networks</topic><topic>Crystallinity</topic><topic>Electrical Engineering</topic><topic>Electrical resistivity</topic><topic>Electron transport</topic><topic>Energy gap</topic><topic>Heterojunctions</topic><topic>Lasers</topic><topic>Mathematical analysis</topic><topic>Optical Devices</topic><topic>Optical properties</topic><topic>Optics</topic><topic>Perovskites</topic><topic>Photonics</topic><topic>Photovoltaic cells</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Solar cells</topic><topic>Spectrophotometry</topic><topic>Spin coating</topic><topic>Spin coatings</topic><topic>X-ray diffraction</topic><topic>Zinc oxide</topic><topic>Zinc oxides</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Koné, Klègayéré Emmanuel</creatorcontrib><creatorcontrib>Bouich, Amal</creatorcontrib><creatorcontrib>Soro, Donafologo</creatorcontrib><creatorcontrib>Soucase, Bernabé Marí</creatorcontrib><collection>CrossRef</collection><jtitle>Optical and quantum electronics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Koné, Klègayéré Emmanuel</au><au>Bouich, Amal</au><au>Soro, Donafologo</au><au>Soucase, Bernabé Marí</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Surface engineering of zinc oxide thin as an electron transport layer for perovskite solar cells</atitle><jtitle>Optical and quantum electronics</jtitle><stitle>Opt Quant Electron</stitle><date>2023-07-01</date><risdate>2023</risdate><volume>55</volume><issue>7</issue><artnum>574</artnum><issn>0306-8919</issn><eissn>1572-817X</eissn><abstract>This work investigates the zinc oxide (ZnO) deposited by the spin coating technique which has for the main advantage of its implementation. Zinc oxide is a semiconductor that has a direct optical bandgap of 3.3 eV which has transparency properties of about 80% optical, anti-reflection in the UV-Vis spectrum, and high electrical conductivity (Cao et al. 2018). The electron transport layer (ETL) is one of its main functions in a solar cell. The number of spin coatings was changed from 1 to 4 in order to get different variations of ZnO thicknesses. These different samples were characterized. X-Ray Diffraction (XRD) showed the polycrystalline character of the ZnO films. Two peaks (the strongest) have been identified on planes (002) and (101). SEM showed that the surface of the samples presents a good crystallinity, which agrees with the results of XRD. Moreover, the crystallinity and the density increase with the number of cycles. The transmittance of samples obtained by spectrophotometry was about 80% in the visible and decreases with the number of cycles. Bandgap was calculated from absorbance data and it varies from 3.25 to 3.29 eV. The best sample was the sample with four cycles (ZnO-4). It was used for heterojunction with mixed halide methylammonium lead (MAPbBr 2 I). The bandgap obtained of the heterojunction MAPbBr 2 I/ZnO-4 was 1.9 eV. The simulation of the mixed halide methylammonium lead (MAPbBr 2 I) base-solar cell resulted in 16.938095 mA/cm 2 , 2 V, and 33.88% for Jsc, Voc, and eta respectively.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s11082-023-04671-6</doi></addata></record>
fulltext fulltext
identifier ISSN: 0306-8919
ispartof Optical and quantum electronics, 2023-07, Vol.55 (7), Article 574
issn 0306-8919
1572-817X
language eng
recordid cdi_proquest_journals_2811673311
source SpringerLink
subjects Characterization and Evaluation of Materials
Computer Communication Networks
Crystallinity
Electrical Engineering
Electrical resistivity
Electron transport
Energy gap
Heterojunctions
Lasers
Mathematical analysis
Optical Devices
Optical properties
Optics
Perovskites
Photonics
Photovoltaic cells
Physics
Physics and Astronomy
Solar cells
Spectrophotometry
Spin coating
Spin coatings
X-ray diffraction
Zinc oxide
Zinc oxides
title Surface engineering of zinc oxide thin as an electron transport layer for perovskite solar cells
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-14T15%3A50%3A51IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Surface%20engineering%20of%20zinc%20oxide%20thin%20as%20an%20electron%20transport%20layer%20for%20perovskite%20solar%20cells&rft.jtitle=Optical%20and%20quantum%20electronics&rft.au=Kon%C3%A9,%20Kl%C3%A8gay%C3%A9r%C3%A9%20Emmanuel&rft.date=2023-07-01&rft.volume=55&rft.issue=7&rft.artnum=574&rft.issn=0306-8919&rft.eissn=1572-817X&rft_id=info:doi/10.1007/s11082-023-04671-6&rft_dat=%3Cproquest_cross%3E2811673311%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=2811673311&rft_id=info:pmid/&rfr_iscdi=true