Abstract
Electron density differences resulting from atom displacement patterns aligned with phonon modes in MgB2 have been calculated using density functional theory (DFT). The extent of phonon anomalies, identified as indicators of the superconducting transition temperature, Tc, under a range of conditions in AlB2-type structures, reduce as boron atoms are displaced from their equilibrium positions along E2g mode directions. The Fermi energy for displacements along the directions of the E2g phonon mode accounts for changes in the covalent B-B bond electronic charge density. We applied differential atom displacements to show that the shifted σ band structure associated with the light effective mass became tangential to the Fermi level and that the Fermi surface undergoes a topological transition at a critical relative displacement of ~0.6% of the boron atoms from equilibrium. The difference in Fermi energies at this critical displacement and at the equilibrium position correspond to the superconducting energy gap. The net volume between tubular σ surfaces in reciprocal space correlated with the depth of the phonon anomaly and, by inference, it is a key to an understanding of superconductivity. This ab initioapproach offers a phenomenological understanding of the factors that determine Tc based on knowledge of the crystal structure.
Highlights
We applied differential atom displacements to show that the shifted σ band structure associated with the light effective mass became tangential to the Fermi level and that the Fermi surface undergoes a topological transition at a critical relative displacement of ~0.6% of the boron atoms from equilibrium
We present modelling outcomes that analyse the impact of atom displacement on phonon modes and on band structure
We have shown that the depth of the phonon dispersion (PD) anomaly provides a temperature which corresponds to the superconducting transition temperature for a wide range of external conditions, accurate within experimental and calculation errors [5] [6] [7] [14]
Summary
For many materials including superconductors, DFT provides facile resolution of fine-scale structural variations (i.e. picometer) because electron density is the key variable in real, three-dimensional coordinate space for a particular crystallography [1]. This fundamental attribute of DFT arises because charge distribution calculations are an explicit feature of these methods [2]. There are many theoretical and experimental studies on MgB2 extant in the literature This abundance of information combined with a simple structure containing two atom types provides an excellent reference for detailed DFT modelling of electron distributions in a conventional BCS superconductor
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