Abstract

The chemical versatility of organic semiconductors provides nearly unlimited opportunities for tuning their electronic properties. However, despite decades of research, the relationship between molecular structure, molecular packing and charge mobility in these materials remains poorly understood. This reduces the search for high-mobility organic semiconductors to the inefficient trial-and-error approach. For clarifying the abovementioned relationship, investigations of the effect of small changes in the chemical structure on organic semiconductor properties are particularly important. In this study, we computationally address the impact of the substitution of C-H atom pairs by nitrogen atoms (N-substitution) on the molecular properties, molecular packing and charge mobility of crystalline oligoacenes. We observe that besides decreasing frontier molecular orbital levels, N-substitution dramatically alters molecular electrostatic potential, yielding pronounced electron-rich and electron-deficient areas. These changes in the molecular electrostatic potential strengthen face-to-face and edge-to-edge interactions in the corresponding crystals and result in the crossover from the herringbone packing motif to π-stacking. When the electron-rich and electron-deficient areas are large, sharply defined and, probably, have a certain symmetry, calculated charge mobility increases up to 3–4 cm2V−1s−1. The results obtained highlight the potential of azaacenes for application in organic electronic devices and are expected to facilitate the rational design of organic semiconductors for the steady improvement of organic electronics.

Highlights

  • Organic semiconductors with efficient charge transport, i.e., high charge mobility μ, are in great demand for organic electronics

  • We have computationally analyzed the effect of the insertion of up to four nitrogen atoms (N-substitution) into the π-conjugated cores of anthracene, tetracene and pentacene

  • It has been found that N-substitution facilitates the π-stacking molecular arrangement in the corresponding crystals that generally results in large charge transfer integrals favorable for charge transport

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Summary

Introduction

Organic semiconductors with efficient charge transport, i.e., high charge mobility μ, are in great demand for organic electronics. The tunability of the molecular structure of OSs [1] gives hope for finding novel high-mobility materials among them. The molecular nature of the OSs limits the charge transport in these materials because charge carriers (electrons or holes) are efficiently delocalized within the molecules, their intermolecular delocalization or transfer from one molecule to another is generally hindered by the weakness of the electronic interaction between the molecules [3,4]. Charge transport proceeds via an inefficient hopping mechanism; the hopping rate increases with J and decreases with λ [5,6,7]. Increasing J and decreasing λ is important for the improvement of charge mobility in OSs

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