Pressure induced magnetic and semiconductor–metal phase transitions in Cr2MoO6
Guo San-Dong†,
       

The magnetization density distributions of Cr2MoO6 at (a) A (AF–F) and (b) F (F–AF) points. The plane is defined by a Cr1–Cr2–Cr3 triangle. The actual magnetization density is −0.01–0.01 |e|/Bohr3 and the density increment is 0.00067 |e|/Bohr3. The blue, black, and red lines stand for positive, negative, and zero values, respectively.