{"title":"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","authors":"Surendra Babu Numbury","doi":"10.1093/oxfmat/itac002","DOIUrl":null,"url":null,"abstract":"\n 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.","PeriodicalId":74385,"journal":{"name":"Oxford open materials science","volume":" ","pages":""},"PeriodicalIF":2.9000,"publicationDate":"2022-04-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"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\",\"authors\":\"Surendra Babu Numbury\",\"doi\":\"10.1093/oxfmat/itac002\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"\\n 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.\",\"PeriodicalId\":74385,\"journal\":{\"name\":\"Oxford open materials science\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":2.9000,\"publicationDate\":\"2022-04-21\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Oxford open materials science\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1093/oxfmat/itac002\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"MATERIALS SCIENCE, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Oxford open materials science","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1093/oxfmat/itac002","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
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.