Competition between the Charge Transfer State and the Singlet States of Donor or Acceptor Limiting the Efficiency in Polymer:Fullerene Solar Cells

被引:230
作者
Faist, Mark A. [1 ,2 ,3 ]
Kirchartz, Thomas [1 ,2 ]
Gong, Wei [1 ,2 ,4 ,5 ]
Ashraf, Raja Shahid [2 ,3 ]
McCulloch, Iain [2 ,3 ]
de Mello, John C. [2 ,3 ]
Ekins-Daukes, Nicholas J. [1 ,2 ]
Bradley, Donal D. C. [1 ,2 ]
Nelson, Jenny [1 ,2 ]
机构
[1] Univ London Imperial Coll Sci Technol & Med, Dept Phys, London SW7 2AZ, England
[2] Univ London Imperial Coll Sci Technol & Med, Ctr Plast Elect, London SW7 2AZ, England
[3] Univ London Imperial Coll Sci Technol & Med, Dept Chem, London SW7 2AZ, England
[4] Beijing Jiaotong Univ, Minist Educ, Key Lab Luminescence & Opt Informat, Beijing 100044, Peoples R China
[5] Beijing Jiaotong Univ, Inst Optoelect Technol, Beijing 100044, Peoples R China
基金
英国工程与自然科学研究理事会;
关键词
OPEN-CIRCUIT VOLTAGE; SELF-ORGANIZATION; TRANSFER EXCITONS; DESIGN RULES; BLEND FILMS; POLYMER; ENERGY; ELECTROLUMINESCENCE; PERFORMANCE; POLY(3-HEXYLTHIOPHENE);
D O I
10.1021/ja210029w
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
We study the appearance and energy of the charge transfer (CT) state using measurements of electroluminescence (EL) and photoluminescence (PL) in blend films of high-performance polymers with fullerene acceptors. EL spectroscopy provides a direct probe of the energy of the interfacial states without the need to rely on the LUMO and HOMO energies as estimated in pristine materials. For each polymer, we use different fullerenes with varying LUMO levels as electron acceptors, in order to vary the energy of the CT state relative to the blend with [6,6]-phenyl C61-butyric acid methyl ester (PCBM). As the energy of the CT state emission approaches the absorption onset of the blend component with the smaller optical bandgap, E-opt,E-min equivalent to min{E-opt,E-donor; E-opt,E-acceptor}, we observe a transition in the EL spectrum from CT emission to singlet emission from the component with the smaller bandgap. The appearance of component singlet emission coincides with reduced photocurrent and fill factor. We conclude that the open circuit voltage V-OC is limited by the smaller bandgap of the two blend components. From the losses of the studied materials, we derive an empirical limit for the open circuit voltage: V-OC less than or similar to E-opt,E-min/e - (0.66 +/- 0.08)eV.
引用
收藏
页码:685 / 692
页数:8
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