高性能有机太阳能电池用A -D - A框架小有机非富勒烯受体分子的设计:DFT和TD-DFT方法

IF 2.9 Q3 MATERIALS SCIENCE, MULTIDISCIPLINARY Oxford open materials science Pub Date : 2022-04-21 DOI:10.1093/oxfmat/itac002
Surendra Babu Numbury
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引用次数: 1

摘要

本研究的主要目的是使用咔唑和苯并噻唑衍生物设计非富勒烯受体A-D-A框架。利用密度泛函理论(DFT)计算了B3LYP泛函在气相和溶剂相中的几何优化结构和电子性质,该泛函具有6-311G的基组。计算了这些受体的前沿分子轨道(FMO)、带隙、开路电压(VOC)和偶极矩。理论紫外吸收光谱由时间相关密度泛函理论(TD-DFT)计算,理论水平与DFT方法相同。它们显示出合适的带隙(2.24–2.93 eV)和偶极矩(1.8–10.8 Debye)。在气体和溶剂中,该范围内所有研究分子的最大波长(λmax)为665.17–679.97。与气相吸收相比,在为氯苯选择的所有受体中都观察到轻微的红移。非富勒烯受体A11具有最低的带隙能量(2.24 eV),气相激发能(1.86 eV)和氯苯激发能(1.86 eV)(1.86 eV)。因此,A11被预测为未来有机非富勒烯受体的有力竞争者。开路电压(Voc)值范围从1.53到2.56 因此,光电子、分子轨道分布以及A11和A12分子是非富勒烯受体的合适受体。
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Designing of small organic non-fullerene(NFAs) acceptor molecules with an A−D−A Framework for high performance organic solar cells: A DFT and TD-DFT method
The main objective of this research was to design non-fullerene acceptors A-D-A framework, using carbazole and benzothiazole derivatives. Density functional theory (DFT) was used to calculate the geometry optimized structures and electronic properties at B3LYP functional with a 6-311G basis set in the gas and solvent phase.The frontier molecular orbital’s (FMO), bandgap, Open-circuit voltage (VOC) and dipole moments of these developed acceptors have been calculated. The theoretical UV absorption spectrawere calculated from Time-Dependent Density Functional Theory (TD-DFT) with the same level of theory used DFT method.They show a suitable bandgap (2.24–2.93 eV) and dipole moment (1.8–10.8 Debye). The maximum wavelength (λmax) for all studied molecules in the range is 665.17–679.97 in both gas and solvent. A slight redshift was observed in all acceptors selected for chlorobenzene compared to gas phase absorption.The non-fullerene acceptor A11 has the lowest bandgap energy (2.24 eV), gas-phase excitation energy (1.86 eV), and chlorobenzene excitation energy (1.86 eV) (1.86 eV). As a result, A11 is predicted to be a good contender for organic non-fullerene acceptors in the future. The open-circuit voltage (Voc) values range from 1.53 to 2.56 eV. Consequently, the optoelectronic, molecular orbital distribution, and A11 and A12 molecules were suitable acceptors for non-fullerene acceptors.
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