M. Pawłowski , M. Maciaszek , P. Zabierowski , P. Tsoulka , N. Barreau , M. Igalson
{"title":"用光致发光技术研究了CuGaSe2的深度缺陷水平","authors":"M. Pawłowski , M. Maciaszek , P. Zabierowski , P. Tsoulka , N. Barreau , M. Igalson","doi":"10.1016/j.solmat.2025.113401","DOIUrl":null,"url":null,"abstract":"<div><div>We present a comprehensive study of photoluminescence spectra of the CuGaSe<sub>2</sub> (CGS) thin films, with a focus on the influence of variation in the copper content on optical transitions involving deep defects. The CGS samples investigated here were grown via the three-stage co-evaporation method, and exhibited varying [Cu]/([Cu]+[Ga]) ratios of 1.01, 0.98, and 0.92. We analyzed only the part of the spectrum below 1.3 eV, and carefully considered the interference effects in the analysis. Two prominent peaks were identified in this low-energy region. The first peak (A), located at 0.98 eV, was present in all samples, regardless of their stoichiometry. The second peak (B) at 1.12 eV emerged exclusively in Cu-poor samples, indicating its dependence on copper stoichiometry. Based on an analysis of the PL spectra, <em>ab initio</em> calculations, and literature data, peaks were tentatively assigned to donor-acceptor radiative recombination involving native defects. We proposed two alternative models to explain the nature of peak A at 0.98 eV. The first model assumed a nonintuitive recombination mechanism due to the V<sub>Se</sub> charge state change by capturing a hole located on V<sub>Cu</sub>. In the second model, we proposed a transition between a deep donor Ga<sub>Cu</sub>(2+/+) and a deep acceptor, which is probably Cu<sub>Ga</sub>(0/-). Peak B at 1.12 eV, within both models, is explained as a recombination between a deep donor, i.e. a substitutional defect Ga<sub>Cu</sub> (2+/+), and a shallow acceptor V<sub>Cu</sub>.</div></div>","PeriodicalId":429,"journal":{"name":"Solar Energy Materials and Solar Cells","volume":"282 ","pages":"Article 113401"},"PeriodicalIF":6.6000,"publicationDate":"2025-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Deep defect levels in CuGaSe2 investigated with photoluminescence\",\"authors\":\"M. Pawłowski , M. Maciaszek , P. Zabierowski , P. Tsoulka , N. Barreau , M. Igalson\",\"doi\":\"10.1016/j.solmat.2025.113401\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>We present a comprehensive study of photoluminescence spectra of the CuGaSe<sub>2</sub> (CGS) thin films, with a focus on the influence of variation in the copper content on optical transitions involving deep defects. The CGS samples investigated here were grown via the three-stage co-evaporation method, and exhibited varying [Cu]/([Cu]+[Ga]) ratios of 1.01, 0.98, and 0.92. We analyzed only the part of the spectrum below 1.3 eV, and carefully considered the interference effects in the analysis. Two prominent peaks were identified in this low-energy region. The first peak (A), located at 0.98 eV, was present in all samples, regardless of their stoichiometry. The second peak (B) at 1.12 eV emerged exclusively in Cu-poor samples, indicating its dependence on copper stoichiometry. Based on an analysis of the PL spectra, <em>ab initio</em> calculations, and literature data, peaks were tentatively assigned to donor-acceptor radiative recombination involving native defects. We proposed two alternative models to explain the nature of peak A at 0.98 eV. The first model assumed a nonintuitive recombination mechanism due to the V<sub>Se</sub> charge state change by capturing a hole located on V<sub>Cu</sub>. In the second model, we proposed a transition between a deep donor Ga<sub>Cu</sub>(2+/+) and a deep acceptor, which is probably Cu<sub>Ga</sub>(0/-). Peak B at 1.12 eV, within both models, is explained as a recombination between a deep donor, i.e. a substitutional defect Ga<sub>Cu</sub> (2+/+), and a shallow acceptor V<sub>Cu</sub>.</div></div>\",\"PeriodicalId\":429,\"journal\":{\"name\":\"Solar Energy Materials and Solar Cells\",\"volume\":\"282 \",\"pages\":\"Article 113401\"},\"PeriodicalIF\":6.6000,\"publicationDate\":\"2025-04-01\",\"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/S0927024825000029\",\"RegionNum\":2,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"2025/1/13 0:00:00\",\"PubModel\":\"Epub\",\"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/S0927024825000029","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2025/1/13 0:00:00","PubModel":"Epub","JCR":"Q2","JCRName":"ENERGY & FUELS","Score":null,"Total":0}
Deep defect levels in CuGaSe2 investigated with photoluminescence
We present a comprehensive study of photoluminescence spectra of the CuGaSe2 (CGS) thin films, with a focus on the influence of variation in the copper content on optical transitions involving deep defects. The CGS samples investigated here were grown via the three-stage co-evaporation method, and exhibited varying [Cu]/([Cu]+[Ga]) ratios of 1.01, 0.98, and 0.92. We analyzed only the part of the spectrum below 1.3 eV, and carefully considered the interference effects in the analysis. Two prominent peaks were identified in this low-energy region. The first peak (A), located at 0.98 eV, was present in all samples, regardless of their stoichiometry. The second peak (B) at 1.12 eV emerged exclusively in Cu-poor samples, indicating its dependence on copper stoichiometry. Based on an analysis of the PL spectra, ab initio calculations, and literature data, peaks were tentatively assigned to donor-acceptor radiative recombination involving native defects. We proposed two alternative models to explain the nature of peak A at 0.98 eV. The first model assumed a nonintuitive recombination mechanism due to the VSe charge state change by capturing a hole located on VCu. In the second model, we proposed a transition between a deep donor GaCu(2+/+) and a deep acceptor, which is probably CuGa(0/-). Peak B at 1.12 eV, within both models, is explained as a recombination between a deep donor, i.e. a substitutional defect GaCu (2+/+), and a shallow acceptor VCu.
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.