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Chemical doping is a key process for controlling the electronic properties of molecular semiconductors, including their conductivity and work function. A common limitation of n-doped polymers is their instability under ambient conditions, which has imposed restrictions on the characterisation and device application of n-doped polymers. In this study, sequential n-doping with organometallic dopants was performed on thin films of polymeric semiconductors with naphthalene diimide and perylene diimide-based backbones. Moderate ambient stability was achieved with (RuCp*Mes) 2 , {Cp* = pentamethylcyclopentadienyl; Mes = 1,3,5-trimethylbenzene}, which is in striking contrast to the unstable, n-doped state obtained with cobaltocene, a simple one-electron reductant. The highly cathodic, effective redox potential of (RuCp*Mes) 2 , ca. −2.0 V vs. ferrocene, suppresses the back electron transfer reaction and the subsequent dopant loss in air, which gives rise to the observed air stability. It also allows a perylene diimide-based polymer to be reduced to a state in which the repeat units are largely dianionic. Photoelectron measurements show that the ionization potential of the heavily doped polymer is ca. 3.9 eV. Our findings show that chemical doping with (RuCp*Mes) 2 is an effective method to produce highly stable, n-doped conjugated polymers. 

Organic semiconductors with distinct molecular properties and large carrier mobilities are constantly developed in attempt to produce highly‐efficient electronic materials. Recently, designer molecules with unique structural modifications have been expressly developed to suppress molecular motions in the solid state that arise from low‐energy phonon modes, which uniquely limit carrier mobilities through electron–phonon coupling. However, such low‐frequency vibrational dynamics often involve complex molecular dynamics, making comprehension of the underlying electronic origins of electron–phonon coupling difficult. In this study, first a mode‐resolved picture of electron–phonon coupling in a series of materials that are specifically designed to suppress detrimental vibrational effects, is generated. From this foundation, a method is developed based on the crystalline orbital Hamiltonian population (COHP) analyses to resolve the origins—down to the single atomic‐orbital scale—of surprisingly large electron–phonon coupling constants of particular vibrations, explicitly detailing the manner in which the intermolecular wavefunction overlap is perturbed. Overall, this approach provides a comprehensive explanation into the unexpected effects of less‐commonly studied molecular vibrations, revealing new aspects of molecular design that should be considered for creating improved organic semiconducting materials.

 

Utilizing the intrinsic mobility–strain relationship in semiconductors is critical for enabling strain engineering applications in high‐performance flexible electronics. Here, measurements of Hall effect and Raman spectra of an organic semiconductor as a function of uniaxial mechanical strain are reported. This study reveals a very strong, anisotropic, and reversible modulation of the intrinsic (trap‐free) charge carrier mobility of single‐crystal rubrene transistors with strain, showing that the effective mobility of organic circuits can be enhanced by up to 100% with only 1% of compressive strain. Consistently, Raman spectroscopy reveals a systematic shift of the low‐frequency Raman modes of rubrene to higher (lower) frequencies with compressive (tensile) strain, which is indicative of a reduction (enhancement) of thermal molecular disorder in the crystal with strain. This study lays the foundation of the strain engineering in organic electronics and advances the knowledge of the relationship between the carrier mobility, low‐frequency vibrational modes, strain, and molecular disorder in organic semiconductors.