Figure 2
From: Robust half-metallicity and magnetic phase transition in Sr2CrReO6 via strain engineering
Calculated GGA/GGA+U spin-polarized (a, a\(^{\prime} \)) total and orbital resolved partial (b, b\(^{\prime} \)) Cr 3d and (c, c\(^{\prime} \)) Re 5d density of states (DOS) of \({\text{Sr}}_2 {\text{CrReO}}_6\) in a FiM spin oredering. (d, d\(^{\prime} \)) represents the spin density difference (difference between spin-majority and spin-minority channels) for the top view in the ac-plane. The same iso-value of \(0.05\textit{e}/{\AA }^3\) is used to produce these spin distribution plots. The Fermi level is shown by the vertical dashed line at 0 eV in each DOS figure. The x, y, and z-axes are along the crystallographic a, b, and c-directions, respectively. The y-axis (b-direction) is pointing towards the observer.
