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Deciphering the Multifarious Charge‐Transport Behaviour of Crystalline Propeller‐Shaped Triphenylamine Analogues
Author(s) -
Ambili R. V.,
Sasikumar Devika,
Hridya P.,
Hariharan Mahesh
Publication year - 2019
Publication title -
chemistry – a european journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.687
H-Index - 242
eISSN - 1521-3765
pISSN - 0947-6539
DOI - 10.1002/chem.201804620
Subject(s) - triphenylamine , intermolecular force , moiety , chemistry , substituent , molecular orbital , atomic orbital , chemical physics , molecule , computational chemistry , crystallography , stereochemistry , electron , photochemistry , physics , quantum mechanics , organic chemistry
Abstract A collection of para ‐substituted propeller‐shaped triphenylamine (TPA) derivatives have been computationally investigated for charge‐transport characteristics exhibited by the derivatives by using the Marcus–Hush formalism. The various substituents chosen herein, with features that range from electron withdrawing to electron donating in nature, play a key role in defining the reorganisation energy and electronic coupling properties of the TPA derivatives. The TPA moiety is expected to possess weak electronic coupling on the basis of poor orbital overlap upon aggregation, owing to the restriction imposed by the propeller shape of the TPA core. However, the substituent groups attached to the TPA core can significantly dictate the crystal‐packing motif of the TPA derivatives, wherein the variety of noncovalent intermolecular interactions subsequently generated drive the packing arrangement and influence electronic coupling between the neighbouring orbitals. Intermolecular interactions in the crystalline architecture of TPA derivatives were probed by using Hirshfeld and quantum theory of atoms‐in‐molecules techniques. Furthermore, symmetry‐adapted perturbation theory analysis of the TPA analogues has revealed that a periodic arrangement of energetically stable dimers with significant electronic coupling is essential to contribute high charge‐carrier mobility to the overall crystal.