Figure 4
From: Thermal equation of state of ruthenium characterized by resistively heated diamond anvil cell

Pressure evolution of the Raman active (E2g) and silent (B1g) modes as obtained from present calculations, compared to previous work39.
From: Thermal equation of state of ruthenium characterized by resistively heated diamond anvil cell

Pressure evolution of the Raman active (E2g) and silent (B1g) modes as obtained from present calculations, compared to previous work39.