On Heavy Carbon Doping of MgB$_2$

TL;DR

This study uses first principles calculations to analyze heavy carbon doping effects in MgB$_2$, revealing how doping alters electronic structure and the $ ext{σ}$-band Fermi surface, impacting superconductivity.

Contribution

It provides detailed computational insights into how heavy carbon doping modifies the electronic structure and Fermi surface of MgB$_2$, a key to understanding doping effects on superconductivity.

Findings

The $ ext{σ}$-bands split by 60 meV at x=0.0833 doping.

The $ ext{σ}$ Fermi cylinders contain 0.070 holes/cell at this doping level.

The $ ext{σ}$ Fermi surface cylinders pinch off at x ~ 0.10 doping.

Abstract

Heavy carbon doping of MgB$_2$ is studied by first principles electronic structure studies of two types, an ordered supercell (Mg(B$_{1-x}$C$_{x}$)$_{2}$,x=0.0833) and also the coherent potential approximation method that incorporates effects of B-C disorder. For the ordered model, the twofold degenerate $\sigma$-bands that are the basis of the high temperature superconductivity are split by 60 meV (i.e.7 meV/%C) and the $\sigma$ Fermi cylinders contain 0.070 holes/cell, compared to 0.11 for MgB$_2$. A virtual crystal treatment tends to overestimate the rate at which $\sigma$ holes are filled by substitutional carbon. The coherent potential approximation (CPA) calculations give the same rate of band filling as the supercell method. The occupied local density of states of C is almost identical to that of B in the upper 2 eV of the valence bands, but in the range -8 eV to -2 eV, C has a considerably larger density of states. The calculations indicate that the $\sigma$ Fermi surface cylinders pinch off at the zone center only above the maximum C concentration x ~ 0.10. These results indicate that Mg(B$_{1-x}$C$_{x}$)$_{2}$ as well as Mg$_{1-x}$Al$_x$B$_2$ is a good system in which to study the evolution of the unusual electron-phonon coupling character and strength as the crucial $\sigma$ hole states are filled.