Our approach uses two coordinates, the number of electrons transferred (ET) and the number of electrons shared (ES) between adjacent atoms. These values are derived from quantum-chemical calculations. An ES value of 2 corresponds to a perfect covalent bond with one electron pair being shared between adjacent atoms, while an ET value of 1 indicates that the valence electrons are fully transferred, forming a perfect ionic bond. This map can separate clearly between classical chemical bonds, such as metallic, covalent and ionic bonds and indicates that another fundamental bonding mechanism exists in solids, which has been coined Metavalent Bonding.
An interactive version of this map has been created to reduce the entry barrier of utilizing our concepts. On startup, the 2D map representation using ES and ET is shown. The view can be rotated by holding down the right mouse button. Left clicking a data point opens a panel with additional information about the material selected. To transition between different map types: 1st generation: van Arkel / Ketelaar; 2nd generation: Philips, van Vechten, Littlewood; 3rd generation (based on ES and ET: our work) the green buttons on the left hand side can be clicked. The blue buttons at the top display various properties on the z-axis. Hovering over a button opens a tooltip with a description of its function.
The preparation of samples with interesting properties is of paramount importance for our team. We either produce thin film samples with the desired stoichiometry and exciting properties by molecular beam epitaxy or sputtering or grow our own single crystals.
Our work builds on the belief that optical properties are governed by the chemical bonds between the atoms involved. Hence, we measure optical properties with high precision using FTIR spectroscopy, spectroscopic ellipsometry as well as UV / VIS spectroscopy.
We need to determine the stoichiometry of our samples with great precision. Yet, beyond this, we also want to determine the atomic arrangement on the nanoscale, enabling us to detect sample inhomogeneities and nanostructures employing atom probe tomography. Needless to say that we also determine the average atomic arrangement with high precision using x-ray and electron diffraction.
We need to determine the stoichiometry of our samples with great precision. Yet, beyond this, we also want to determine the atomic arrangement on the nanoscale, enabling us to detect sample inhomogeneities and nanostructures employing atom probe tomography. Needless to say that we also determine the average atomic arrangement with high precision using x-ray and electron diffraction.