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M. Kemerink

Publications and source records attributed to M. Kemerink.

4 recordsLinked to original sources

A supramolecular ferroelectric with two sublattices and polarization dependent conductivity

The possibility to combine and finetune properties of functional molecular materials by chemical design is particularly relevant for organic ferroelectrics. In this work, we investigate a class of organic molecular materials that show long-range supramolecular organization into fibrillar bundles. In solid state, the material shows ferroelectric behavior resulting from two largely independent dipolar moieties that show up as two separate coercive fields in polarization-hysteresis and capacitance-voltage curves. Moreover, the material shows a long-range electronic conductivity that arises due to oxidation at the positive electrode, followed by electron transfer between neighboring molecules. We find that this conductivity is modulated by the direction and degree of ferroelectric polarization, which we interpret in terms of injection barrier modulation at low electric fields and a recently developed framework for asymmetric polaron hopping at high fields. With two distinct, partially independent dipolar moieties offering the possibility to use ferroelectric properties to modulate conductance, the materials presented herein are a promising basis for multifunctional materials.

cond-mat.mtrl-sci

Highly polar groups and supramolecular order enable charge injection and long-range conductivity in organic materials without extended {\pi}-systems

Electronic conductivity in organic materials is well-established. Both semiconductive and metallic behavior is observed in (quasi) 0-, 1-, 2- and 3-dimensional carbon-based materials and is applied in a wide range of commercial devices. Despite their large structural variety, these materials commonly have an extended {\pi}-system, formed by a double-digit number of conjugated sp2-hybridized carbon atoms, which is responsible for the conductivity. Here, we present a class of organic molecular materials that, despite the absence of an extended {\pi}-system, show a distinct direct current conductivity in quasi-1D supramolecular stacks of small organic molecules. Long-range conductivity takes place by removal of an electron from the highest occupied molecular orbital, i.e. oxidation, followed by charge transfer between neighboring molecules. Kelvin probe force microscopy (KPFM) on thin-film devices shows that the resulting transport band only becomes energetically accessible for charge injection from the contacts thanks to interfacial dipoles that shift the relevant molecular orbital levels by up to 2 eV. Long-range order in the form of fibrillar supramolecular polymers with lengths exceeding several micrometers enhances the macroscopic conductivity but is not essential. While current densities are moderate, this work provides a compelling explanation for the existing body of knowledge on non-{\pi}-conjugated conductivity and suggests a new way to endow organic materials with conductivity.

cond-mat.mtrl-sci

Influence of the Characteristics of the STM-tip on the Electroluminescence Spectra

We analyze the influence of the characteristics of the STM-tip (applied voltage, tip radius) on the electroluminescence spectra from an STM-tip-induced quantum dot taking into account the many-body effects. We find that positions of electroluminescence peaks, attributed to the electron-hole recombination in the quantum dot, are very sensitive to the shape and size of the confinement potential as determined by the tip radius and the applied voltage. A critical value of the tip radius is found, at which the luminescence peak positions as a function of the tip radius manifest a transition from decreasing behavior for smaller radii to increasing behavior for larger radii. We find that this critical value of the tip radius is related to the confinement in the lateral and normal direction.

cond-mat.mes-hall

Scaling Of The Coulomb Energy Due To Quantum Fluctuations In The Charge Of A Quantum Dot

The charging energy of a quantum dot is measured through the effect of its potential on the conductance of a second dot. This technique allows a measurement of the scaling of the dot's charging energy with the conductance of the tunnel barriers leading to the dot. We find that the charging energy scales quadratically with the reflection probability of the barriers. In a second experiment we study the transition from a single to a double-dot which exhibits a scaling behavior linear in the reflection probability. The observed power-laws agree with a recent theory.

cond-mat