Zinnia Mallick, Sudip Naskar, Shanker Ram and Dipankar Mandal
{"title":"Light-regulated pyro-phototronic effects in a perovskite Cs2SnI6-reinforced ferroelectric polymer hybrid nanostructure†","authors":"Zinnia Mallick, Sudip Naskar, Shanker Ram and Dipankar Mandal","doi":"10.1039/D4MH01198H","DOIUrl":null,"url":null,"abstract":"<p >The ‘pyro-phototronic effect’ plays a nontrivial role in advancing ferroelectric (FE) devices of light detectors, light-emitting diodes, and other smart technologies. In this work, a premier FE copolymer, poly(vinylidene fluoride-<em>co</em>-trifluoro ethylene) (P(VDF-TrFE)), is reinforced with a lead-free double perovskite, Cs<small><sub>2</sub></small>SnI<small><sub>6</sub></small>, to render profound properties in a hybrid nanostructure. It presents a unique example of the coupling of ferro-, pyro- and piezo-electrics to the ‘photoexcitation’ of exotic charges that actively empower the synergetic features. Cs<small><sub>2</sub></small>SnI<small><sub>6</sub></small> embodied in small crystallites therein is distorted in a non-centrosymmetric class of a rhomboid crystal structure (a new phase) rather than a well-known centrosymmetric face-centred cubic (fcc) phase. It boosts the emerging phototronic properties. A systematic study of the bulk heterojunction reveals the four-stage pyro-phototronic response of transient photocurrent under visible light illumination of a solar simulator (intensity ∼100 mW cm<small><sup>−2</sup></small>). Illumination at a frequency of 0.025 Hz induces a temporal temperature change, Δ<em>T</em> → 3.1 K, in the system, leading to induced pyroelectricity in an integrated circuit. The rise time and response time for the heterojunction are observed as ∼326 ms and ∼225 ms, respectively. The output pyro-phototronic current increases as Δ<em>T</em> increases in an on–off cycle. As a result, the integrated pyro-phototronic effect can be utilized to empower optoelectronic devices and harvest stray ‘thermal energy’ for running small energy devices.</p>","PeriodicalId":87,"journal":{"name":"Materials Horizons","volume":" 5","pages":" 1532-1546"},"PeriodicalIF":12.2000,"publicationDate":"2024-11-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Materials Horizons","FirstCategoryId":"88","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2025/mh/d4mh01198h","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
The ‘pyro-phototronic effect’ plays a nontrivial role in advancing ferroelectric (FE) devices of light detectors, light-emitting diodes, and other smart technologies. In this work, a premier FE copolymer, poly(vinylidene fluoride-co-trifluoro ethylene) (P(VDF-TrFE)), is reinforced with a lead-free double perovskite, Cs2SnI6, to render profound properties in a hybrid nanostructure. It presents a unique example of the coupling of ferro-, pyro- and piezo-electrics to the ‘photoexcitation’ of exotic charges that actively empower the synergetic features. Cs2SnI6 embodied in small crystallites therein is distorted in a non-centrosymmetric class of a rhomboid crystal structure (a new phase) rather than a well-known centrosymmetric face-centred cubic (fcc) phase. It boosts the emerging phototronic properties. A systematic study of the bulk heterojunction reveals the four-stage pyro-phototronic response of transient photocurrent under visible light illumination of a solar simulator (intensity ∼100 mW cm−2). Illumination at a frequency of 0.025 Hz induces a temporal temperature change, ΔT → 3.1 K, in the system, leading to induced pyroelectricity in an integrated circuit. The rise time and response time for the heterojunction are observed as ∼326 ms and ∼225 ms, respectively. The output pyro-phototronic current increases as ΔT increases in an on–off cycle. As a result, the integrated pyro-phototronic effect can be utilized to empower optoelectronic devices and harvest stray ‘thermal energy’ for running small energy devices.