{"title":"外延 BiFeO3/La0.5Sr0.5CO3 异质结构中的结构和铁电光伏效应调制","authors":"","doi":"10.1016/j.micrna.2024.207956","DOIUrl":null,"url":null,"abstract":"<div><p>Square-shaped BiFeO<sub>3</sub> (BFO) thin films were prepared on SrTiO<sub>3</sub> (STO) substrates by off-axis magnetron sputtering using La<sub>0.5</sub>Sr<sub>0.5</sub>CoO<sub>3</sub> (LSCO) as the bottom electrode, and both LSCO and BFO are perovskite structure. The BFO crystalline quality improves and the grain size becomes larger as the thickness H increases, and both have smaller mean square roughness. The effects of BFO thickness H, light intensity I<sub>p</sub> and ambient temperature AT on the ferroelectric photovoltaic effect (FPE) for the Pt/BFO/LSCO heterostructures are significant. With the H increase, the open-circuit voltage V<sub>oc</sub> and short-circuit current J<sub>sc</sub> increase linearly, with V<sub>oc</sub> up to 0.44 V. The short-circuit current modulation intensity ΔJ<sub>sc</sub> follows the ΔJ<sub>sc-300</sub>>ΔJ<sub>sc-200</sub>>ΔJ<sub>sc-100</sub> rule. With the I<sub>p</sub> increase, Pt/BFO(300 nm)/LSCO’ J<sub>sc</sub> increases linearly, and V<sub>oc</sub> first increases and then tends to saturation, which satisfies Glass' law. With the AT increases, V<sub>oc</sub> is linearly decreasing and J<sub>sc</sub> shows the law: decreasing→increasing→decreasing. The polarization-modulated FPE mechanism is investigated by analyzing the Pt/BFO/LSCO energy band structure, which is attributed to the coupling effect between the BFO depolarization field (E<sub>dp</sub>) and the built-in electric field at the interface (E<sub>Pt/BFO</sub> & E<sub>BFO/LSCO</sub>), and the FPE mechanism is shifted from the interface barrier domination to the ferroelectric polarization domination as H increases.</p></div>","PeriodicalId":100923,"journal":{"name":"Micro and Nanostructures","volume":null,"pages":null},"PeriodicalIF":2.7000,"publicationDate":"2024-08-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Structure and ferroelectric photovoltaic effect modulation in the epitaxial BiFeO3/La0.5Sr0.5CO3 heterostructures\",\"authors\":\"\",\"doi\":\"10.1016/j.micrna.2024.207956\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Square-shaped BiFeO<sub>3</sub> (BFO) thin films were prepared on SrTiO<sub>3</sub> (STO) substrates by off-axis magnetron sputtering using La<sub>0.5</sub>Sr<sub>0.5</sub>CoO<sub>3</sub> (LSCO) as the bottom electrode, and both LSCO and BFO are perovskite structure. The BFO crystalline quality improves and the grain size becomes larger as the thickness H increases, and both have smaller mean square roughness. The effects of BFO thickness H, light intensity I<sub>p</sub> and ambient temperature AT on the ferroelectric photovoltaic effect (FPE) for the Pt/BFO/LSCO heterostructures are significant. With the H increase, the open-circuit voltage V<sub>oc</sub> and short-circuit current J<sub>sc</sub> increase linearly, with V<sub>oc</sub> up to 0.44 V. The short-circuit current modulation intensity ΔJ<sub>sc</sub> follows the ΔJ<sub>sc-300</sub>>ΔJ<sub>sc-200</sub>>ΔJ<sub>sc-100</sub> rule. With the I<sub>p</sub> increase, Pt/BFO(300 nm)/LSCO’ J<sub>sc</sub> increases linearly, and V<sub>oc</sub> first increases and then tends to saturation, which satisfies Glass' law. With the AT increases, V<sub>oc</sub> is linearly decreasing and J<sub>sc</sub> shows the law: decreasing→increasing→decreasing. The polarization-modulated FPE mechanism is investigated by analyzing the Pt/BFO/LSCO energy band structure, which is attributed to the coupling effect between the BFO depolarization field (E<sub>dp</sub>) and the built-in electric field at the interface (E<sub>Pt/BFO</sub> & E<sub>BFO/LSCO</sub>), and the FPE mechanism is shifted from the interface barrier domination to the ferroelectric polarization domination as H increases.</p></div>\",\"PeriodicalId\":100923,\"journal\":{\"name\":\"Micro and Nanostructures\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":2.7000,\"publicationDate\":\"2024-08-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Micro and Nanostructures\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S277301232400205X\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, CONDENSED MATTER\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Micro and Nanostructures","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S277301232400205X","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, CONDENSED MATTER","Score":null,"Total":0}
引用次数: 0
摘要
以 La0.5Sr0.5CoO3(LSCO)为底电极,通过离轴磁控溅射法在 SrTiO3(STO)衬底上制备了方形 BiFeO3(BFO)薄膜,LSCO 和 BFO 均为包晶结构。随着厚度 H 的增加,BFO 的结晶质量提高,晶粒尺寸变大,且二者的均方粗糙度都较小。BFO 厚度 H、光照强度 Ip 和环境温度 AT 对 Pt/BFO/LSCO 异质结构的铁电光伏效应(FPE)有显著影响。随着 H 的增加,开路电压 Voc 和短路电流 Jsc 呈线性增加,其中 Voc 最高可达 0.44 V;短路电流调制强度 ΔJsc 遵循 ΔJsc-300>ΔJsc-200>ΔJsc-100 规律。随着 Ip 的增加,Pt/BFO(300 nm)/LSCO' Jsc 线性增加,Voc 先增加后趋于饱和,符合格拉斯定律。随着 AT 的增加,Voc 呈线性下降,Jsc 呈下降→增加→减少的规律。通过分析 Pt/BFO/LSCO 能带结构,研究了极化调制 FPE 机制,该机制归因于 BFO 去极化场(Edp)与界面内置电场(EPt/BFO & EBFO/LSCO)之间的耦合效应,随着 H 的增加,FPE 机制从界面势垒主导转向铁电极化主导。
Structure and ferroelectric photovoltaic effect modulation in the epitaxial BiFeO3/La0.5Sr0.5CO3 heterostructures
Square-shaped BiFeO3 (BFO) thin films were prepared on SrTiO3 (STO) substrates by off-axis magnetron sputtering using La0.5Sr0.5CoO3 (LSCO) as the bottom electrode, and both LSCO and BFO are perovskite structure. The BFO crystalline quality improves and the grain size becomes larger as the thickness H increases, and both have smaller mean square roughness. The effects of BFO thickness H, light intensity Ip and ambient temperature AT on the ferroelectric photovoltaic effect (FPE) for the Pt/BFO/LSCO heterostructures are significant. With the H increase, the open-circuit voltage Voc and short-circuit current Jsc increase linearly, with Voc up to 0.44 V. The short-circuit current modulation intensity ΔJsc follows the ΔJsc-300>ΔJsc-200>ΔJsc-100 rule. With the Ip increase, Pt/BFO(300 nm)/LSCO’ Jsc increases linearly, and Voc first increases and then tends to saturation, which satisfies Glass' law. With the AT increases, Voc is linearly decreasing and Jsc shows the law: decreasing→increasing→decreasing. The polarization-modulated FPE mechanism is investigated by analyzing the Pt/BFO/LSCO energy band structure, which is attributed to the coupling effect between the BFO depolarization field (Edp) and the built-in electric field at the interface (EPt/BFO & EBFO/LSCO), and the FPE mechanism is shifted from the interface barrier domination to the ferroelectric polarization domination as H increases.