| Autor: |
Lee D; Department of Semiconductor Physics and EHSRC, University of Ulsan, Ulsan 44610, Republic of Korea., Kim DH; Department of Semiconductor Physics and EHSRC, University of Ulsan, Ulsan 44610, Republic of Korea., Oh CM; Advanced Photonics Research Institute, Gwangju Institute of Science and Technology, Gwangju 61005, Republic of Korea., Park S; Department of Semiconductor Physics and EHSRC, University of Ulsan, Ulsan 44610, Republic of Korea., Krishna NV; Department of Energy Engineering, School of Energy and Chemical Engineering, Ulsan National Institute of Science and Technology (UNIST), Ulsan 44919, Republic of Korea., Wibowo FTA; Department of Energy Engineering, School of Energy and Chemical Engineering, Ulsan National Institute of Science and Technology (UNIST), Ulsan 44919, Republic of Korea., Hwang IW; Advanced Photonics Research Institute, Gwangju Institute of Science and Technology, Gwangju 61005, Republic of Korea., Jang SY; Department of Energy Engineering, School of Energy and Chemical Engineering, Ulsan National Institute of Science and Technology (UNIST), Ulsan 44919, Republic of Korea., Cho S; Department of Semiconductor Physics and EHSRC, University of Ulsan, Ulsan 44610, Republic of Korea. |
| Abstrakt: |
In conventional fullerene-based organic photovoltaics (OPVs), in which the excited electrons from the donor are transferred to the acceptor, the electron charge transfer state ( e E CT ) that electrons pass through has a great influence on the device's performance. In a bulk-heterojunction (BHJ) system based on a low bandgap non-fullerene acceptor (NFA), however, a hole charge transfer state ( h E CT ) from the acceptor to the donor has a greater influence on the device's performance. The accurate determination of h E CT is essential for achieving further enhancement in the performance of non-fullerene organic solar cells. However, the discovery of a method to determine the exact h E CT remains an open challenge. Here, we suggest a simple method to determine the exact h E CT level via deconvolution of the EL spectrum of the BHJ blend (EL B ). To generalize, we have applied our EL B deconvolution method to nine different BHJ systems consisting of the combination of three donor polymers (PM6, PBDTTPD-HT, PTB7-Th) and three NFAs (Y6, IDIC, IEICO-4F). Under the conditions that (i) absorption of the donor and acceptor are separated sufficiently, and (ii) the onset part of the external quantum efficiency (EQE) is formed solely by the contribution of the acceptor only, EL B can be deconvoluted into the contribution of the singlet recombination of the acceptor and the radiative recombination via h E CT . Through the deconvolution of EL B , we have clearly decided which part of the broad EL B spectrum should be used to apply the Marcus theory. Accurate determination of h E CT is expected to be of great help in fine-tuning the energy level of donor polymers and NFAs by understanding the charge transfer mechanism clearly. |
