{"title":"TD-DFT investigation of small molecular donors for enhanced organic photovoltaics","authors":"A. Arunkumar, Xue-Hai Ju, Adeel Mubarik","doi":"10.1007/s11082-025-08454-z","DOIUrl":null,"url":null,"abstract":"<div><p>Many researchers are becoming interested in using metal-free organic compounds (especially donor molecules) in photovoltaic (PV) devices nowadays. Considering the (E)-6-(benzofuran-2-yl)-3-(6-(benzofuran-2-yl)-1-(2-ethylhexyl)-2-oxoindolin-3-ylidene)-1-(2-ethylhexyl)indolin-2-one (IBF), seven new donor–acceptor–donor (D–A–D) with small molecular donors (SMDs) (IBF-D1 to IBF-D7) are designed and investigated for organic solar cells (OSCs) using density functional theory (DFT) and time-dependent DFT (TD-DFT) methods. With the MPW1PW91 functional and the 3-21G basis set being chosen, the theoretically calculated wavelengths (<i>λ</i><sub><i>max</i></sub>) are presented. The molecular orbitals (MOs) energy gaps (<i>E</i><sub><i>g</i></sub>) of the compounds have values ranging from 2.22 to 2.42 eV. Specifically, the lowest <i>E</i><sub><i>g</i></sub> values are found in IBF-D1 (2.25 eV) and IBF-D6 (2.22 eV). Compared to IBF (2.19 eV), IBF-D2 and IBF-D7 show lower excitation energy differences (<i>E</i><sub><i>x</i></sub>). The derivatives (IBF-D1, IBF-D3, IBF-D4, IBF-D5, and IBF-D6) have the highest <i>λ</i><sub><i>max</i></sub> values compared to IBF. The reorganization energies (RE) are between 0.0125–0.0195 eV for electron (<i>λ</i><sub><i>e</i></sub>) and 0.0019–0.0115 eV for hole mobilities (<i>λ</i><sub><i>h</i></sub>). Additional support for these findings comes from measurements of the transition density matrix (TDM) and molecular electrostatic potential (MEP). Compared to IBF (1.22 eV), IBF-D1 (1.24 eV), IBF-D4 (1.23 eV), and IBF-D6 (1.26 eV) have the highest open circuit voltage (<i>V</i><sub><i>oc</i></sub>). The power conversion efficiency (<i>PCE</i>) values range from 0.83 to 1.13 %. In particular, IBF-D1 (1.11%) and IBF-D6 (1.13%) are superior <i>PCEs</i> of the OSCs. The nonlinear optical (NLO) parameters of the dipole moment (<i>µ</i>), polarizability (<i>α</i>), and first-order hyperpolarizability (<i>β</i>) for the molecules IBF-D1 (<i>µ</i> = 1.08 D, <i>β</i> = 1.70 esu, <i>α</i> = 5.00 esu) and IBF-D6 (<i>µ</i> = 3.40 D, <i>α</i> = 5.08 esu, <i>β</i> = 2.44 esu, respectively) are higher than those of IBF (<i>µ</i> = 0.84 D, <i>α</i> = 4.42 esu, <i>β</i> = 0.07 esu)<i>.</i> Finally, IBF-D1 and IBF-D6 are highly advised to design organic PV with remarkable performance for the optoelectronic devices.</p></div>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":"57 10","pages":""},"PeriodicalIF":4.0000,"publicationDate":"2025-09-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Optical and Quantum Electronics","FirstCategoryId":"5","ListUrlMain":"https://link.springer.com/article/10.1007/s11082-025-08454-z","RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
引用次数: 0
Abstract
Many researchers are becoming interested in using metal-free organic compounds (especially donor molecules) in photovoltaic (PV) devices nowadays. Considering the (E)-6-(benzofuran-2-yl)-3-(6-(benzofuran-2-yl)-1-(2-ethylhexyl)-2-oxoindolin-3-ylidene)-1-(2-ethylhexyl)indolin-2-one (IBF), seven new donor–acceptor–donor (D–A–D) with small molecular donors (SMDs) (IBF-D1 to IBF-D7) are designed and investigated for organic solar cells (OSCs) using density functional theory (DFT) and time-dependent DFT (TD-DFT) methods. With the MPW1PW91 functional and the 3-21G basis set being chosen, the theoretically calculated wavelengths (λmax) are presented. The molecular orbitals (MOs) energy gaps (Eg) of the compounds have values ranging from 2.22 to 2.42 eV. Specifically, the lowest Eg values are found in IBF-D1 (2.25 eV) and IBF-D6 (2.22 eV). Compared to IBF (2.19 eV), IBF-D2 and IBF-D7 show lower excitation energy differences (Ex). The derivatives (IBF-D1, IBF-D3, IBF-D4, IBF-D5, and IBF-D6) have the highest λmax values compared to IBF. The reorganization energies (RE) are between 0.0125–0.0195 eV for electron (λe) and 0.0019–0.0115 eV for hole mobilities (λh). Additional support for these findings comes from measurements of the transition density matrix (TDM) and molecular electrostatic potential (MEP). Compared to IBF (1.22 eV), IBF-D1 (1.24 eV), IBF-D4 (1.23 eV), and IBF-D6 (1.26 eV) have the highest open circuit voltage (Voc). The power conversion efficiency (PCE) values range from 0.83 to 1.13 %. In particular, IBF-D1 (1.11%) and IBF-D6 (1.13%) are superior PCEs of the OSCs. The nonlinear optical (NLO) parameters of the dipole moment (µ), polarizability (α), and first-order hyperpolarizability (β) for the molecules IBF-D1 (µ = 1.08 D, β = 1.70 esu, α = 5.00 esu) and IBF-D6 (µ = 3.40 D, α = 5.08 esu, β = 2.44 esu, respectively) are higher than those of IBF (µ = 0.84 D, α = 4.42 esu, β = 0.07 esu). Finally, IBF-D1 and IBF-D6 are highly advised to design organic PV with remarkable performance for the optoelectronic devices.
期刊介绍:
Optical and Quantum Electronics provides an international forum for the publication of original research papers, tutorial reviews and letters in such fields as optical physics, optical engineering and optoelectronics. Special issues are published on topics of current interest.
Optical and Quantum Electronics is published monthly. It is concerned with the technology and physics of optical systems, components and devices, i.e., with topics such as: optical fibres; semiconductor lasers and LEDs; light detection and imaging devices; nanophotonics; photonic integration and optoelectronic integrated circuits; silicon photonics; displays; optical communications from devices to systems; materials for photonics (e.g. semiconductors, glasses, graphene); the physics and simulation of optical devices and systems; nanotechnologies in photonics (including engineered nano-structures such as photonic crystals, sub-wavelength photonic structures, metamaterials, and plasmonics); advanced quantum and optoelectronic applications (e.g. quantum computing, memory and communications, quantum sensing and quantum dots); photonic sensors and bio-sensors; Terahertz phenomena; non-linear optics and ultrafast phenomena; green photonics.