Exploring seebeck-coefficient fluctuations in endohedral-fullerene, single-molecule junctions.
Ali Khalid IsmaelLaura Rincón-GarcíaCharalambos EvangeliPanagiotis DallasTurki AlotaibiAlaa A Al-JoboryGabino Rubio-BollingerKyriakos PorfyrakisNicolás AgraïtColin J LambertPublished in: Nanoscale horizons (2022)
For the purpose of creating single-molecule junctions, which can convert a temperature difference Δ T into a voltage Δ V via the Seebeck effect, it is of interest to screen molecules for their potential to deliver high values of the Seebeck coefficient S = -Δ V /Δ T . Here we demonstrate that insight into molecular-scale thermoelectricity can be obtained by examining the widths and extreme values of Seebeck histograms. Using a combination of experimental scanning-tunnelling-microscopy-based transport measurements and density-functional-theory-based transport calculations, we study the electrical conductance and Seebeck coefficient of three endohedral metallofullerenes (EMFs) Sc 3 N@C 80 , Sc 3 C 2 @C 80 , and Er 3 N@C 80 , which based on their structures, are selected to exhibit different degrees of charge inhomogeneity and geometrical disorder within a junction. We demonstrate that standard deviations in the Seebeck coefficient σ S of EMF-based junctions are correlated with the geometric standard deviation σ and the charge inhomogeneity σ q . We benchmark these molecules against C 60 and demonstrate that both σ q , σ S are the largest for Sc 3 C 2 @C 80 , both are the smallest for C 60 and for the other EMFs, they follow the order Sc 3 C 2 @C 80 > Sc 3 N@C 80 > Er 3 N@C 80 > C 60 . A large value of σ S is a sign that a molecule can exhibit a wide range of Seebeck coefficients, which means that if orientations corresponding to high values can be selected and controlled, then the molecule has the potential to exhibit high-performance thermoelectricity. For the EMFs studied here, large values of σ S are associated with distributions of Seebeck coefficients containing both positive and negative signs, which reveals that all these EMFs are bi-thermoelectric materials.
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