{"title":"Large bulk photovoltaic effect and Fermi-surface-mediated enhancement with chemical potential in ZnGeP<sub>2</sub>.","authors":"Banasree Sadhukhan","doi":"10.1088/1361-648X/adbb48","DOIUrl":null,"url":null,"abstract":"<p><p>Bulk photovoltaic effect is a non-linear response in noncentrosymmetric materials that converts light into DC current. In this work, we investigate the optical linear and non-linear responses in a chalcopyrite semiconductor ZnGeP<sub>2</sub>. The reference point for chemical potential (E<sub><i>f</i></sub>) appears at the valence band maximum of high symmetry Γ point in Brillouin zone for ZnGeP<sub>2</sub>. We report large bulk photovoltaic namely shift and circular photogalvanic current conductivities which are 4.46<i>µ</i>A V<sup>-2</sup>and -5.49<i>µ</i>A V<sup>-2</sup>respectively with the incident photo energy around ∼5 eV at the chemical potential of<i>E<sub>f</sub></i>= 0 eV which increase about 38% and 81% respectively at a chemical potential of<i>E<sub>f</sub></i>= 1.52 eV. The systematic evolution of the bulk Fermi surface along with the high symmetry points in three dimensional Brillouin zone reveals the enhancement of bulk photovoltaic with the chemical potential in ZnGeP<sub>2</sub>. We further explore the distribution of bulk projected band and surface Fermi surface distribution in the energy landscape using tight binding Hamiltonian within semi infinite slab geometry. The augmentation of bulk photovoltaic with the chemical potential is due to the projected bulk bands along the high symmetryΓ-Zdirection in Brillouin zone. Our thorough and detailed study not only provide a deeper understanding about the role of Fermi surface contribution to the bulk photovoltaic responses with chemical potential, but also suggest ZnGeP<sub>2</sub>as an ideal candidate for optoelectronics and bulk photovoltaic.</p>","PeriodicalId":16776,"journal":{"name":"Journal of Physics: Condensed Matter","volume":" ","pages":""},"PeriodicalIF":2.3000,"publicationDate":"2025-03-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics: Condensed Matter","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1088/1361-648X/adbb48","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, CONDENSED MATTER","Score":null,"Total":0}
引用次数: 0
Abstract
Bulk photovoltaic effect is a non-linear response in noncentrosymmetric materials that converts light into DC current. In this work, we investigate the optical linear and non-linear responses in a chalcopyrite semiconductor ZnGeP2. The reference point for chemical potential (Ef) appears at the valence band maximum of high symmetry Γ point in Brillouin zone for ZnGeP2. We report large bulk photovoltaic namely shift and circular photogalvanic current conductivities which are 4.46µA V-2and -5.49µA V-2respectively with the incident photo energy around ∼5 eV at the chemical potential ofEf= 0 eV which increase about 38% and 81% respectively at a chemical potential ofEf= 1.52 eV. The systematic evolution of the bulk Fermi surface along with the high symmetry points in three dimensional Brillouin zone reveals the enhancement of bulk photovoltaic with the chemical potential in ZnGeP2. We further explore the distribution of bulk projected band and surface Fermi surface distribution in the energy landscape using tight binding Hamiltonian within semi infinite slab geometry. The augmentation of bulk photovoltaic with the chemical potential is due to the projected bulk bands along the high symmetryΓ-Zdirection in Brillouin zone. Our thorough and detailed study not only provide a deeper understanding about the role of Fermi surface contribution to the bulk photovoltaic responses with chemical potential, but also suggest ZnGeP2as an ideal candidate for optoelectronics and bulk photovoltaic.
期刊介绍:
Journal of Physics: Condensed Matter covers the whole of condensed matter physics including soft condensed matter and nanostructures. Papers may report experimental, theoretical and simulation studies. Note that papers must contain fundamental condensed matter science: papers reporting methods of materials preparation or properties of materials without novel condensed matter content will not be accepted.