Abstract

Intrinsic organic small molecule and polymer materials are insulators. The discovery that polymers can be made highly conductive by doping has therefore sparked strong interest in this novel class of conductors. More recently, efficient doping of small molecule materials has also been achieved and is now a key technology in the multi-billion dollar organic light emitting diode industry. Nevertheless, a comprehensive description of charge transport in the presence of doping is still missing for organic semiconductors with localized electronic states. Here, we present a theoretical and computational approach based on percolation theory and quantitatively predict experimental results from the literature for the archetype small molecule materials ZnPc, F8ZnPc and C60. We show that transport in the complex potential landscape that emerges from the presence of localized charges can be aptly analyzed by focusing on the network properties of transport paths instead of just the critical resistance. Specifically, we compute the activation energy of conductivity and the Seebeck energy and yield excellent agreement with experimental data. The previously unexplained increase of the activation energy at high doping concentrations can be clarified by our approach.

Highlights

  • Intrinsic organic small molecule and polymer materials are insulators

  • We concentrate on the charge transport, given the doping charge transfer (CT) was successful

  • We present a comprehensive analysis of hopping transport in doped molecular semiconductor based on percolation theory and variable-range hopping (VRH)

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Summary

Introduction

Intrinsic organic small molecule and polymer materials are insulators. The discovery that polymers can be made highly conductive by doping has sparked strong interest in this novel class of conductors. A comprehensive description of charge transport in the presence of doping is still missing for organic semiconductors with localized electronic states. An example is the influence of the Coulomb potentials of dopants and charge carriers on the nature of charge transport While these potentials exist in doped inorganic semiconductors, there is an important difference: Charge carrier states in organic semiconductors are strongly localized in many cases[16,17,18]. This leads to weaker screening and complex potential landscapes with strong spatial correlations[10,19,20]. What is the mode of charge transport, which paths will carriers take, what are the important length scales? What effect will a certain doping concentration have on a given material?

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