Charge Carrier Formation following Energy Gap Law in Photo-Activated Organic Materials for Efficient Solar Cells

Author:

Rana Aniket123ORCID,Vashistha Nikita34,Kumar Amit35,Kumar Mahesh36ORCID,Singh Rajiv K.35

Affiliation:

1. Department of Chemistry, Imperial College London, London W12 0BZ, UK

2. Centre for Processable Electronics, Imperial College London, London SW7 2AZ, UK

3. Academy of Scientific and Innovative Research (AcSIR), CSIR-NPL Campus, New Delhi 110012, India

4. Institute of Physical Chemistry, Friedrich Schiller University Jena, Helmholtzweg, 4, 07743 Jena, Germany

5. CSIR—National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India

6. Innovation and Management Directorate Council of Scientific and Industrial Research, Anusandhan Bhawan, New Delhi 110001, India

Abstract

The charge carrier formation and transport in the pristine polymers as well as in the polymer–fullerene blend is still a hot topic of discussion for the scientific community. In the present work, the carrier generation in some prominent organic molecules has been studied through ultrafast transient absorption spectroscopy. The identification of the exciton and polaron lifetimes of these polymers has led to device performance-related understanding. In the Energy Gap Law, the slope of the linear fit gradient (γ) of lifetimes vs. bandgap are subjected to the geometrical rearrangements experienced by the polymers during the non-radiative decay from the excited state to the ground state. The value of gradient (γ) for excitons and polarons is found to be −1.1 eV−1 and 1.14 eV−1, respectively. It suggests that the exciton decay to the ground state is likely to involve a high distortion in polymer equilibrium geometry. This observation supports the basis of Stokes shift found in the conjugated polymers due to the high disorder. It provides the possible reasons for the substantial variation in the exciton lifetime. As the bandgap becomes larger, exciton decay rate tends to reduce due to the weak attraction between the holes in the HUMO and electron in the LUMO. The precise inverse action is observed for the polymer–fullerene blend, as the decay of polaron tends to increase as the bandgap of polymer increases.

Publisher

MDPI AG

Reference45 articles.

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