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Activation energy of metastable amorphous Ge \textlesssub\textgreater2\textless/sub\textgreater Sb \textlesssub\textgreater2\textless/sub\textgreater Te \textlesssub\textgreater5\textless/sub\textgreater from room temperature to melt

, , , , , , , , , and . AIP Advances, 8 (6): 065314 (2018)
DOI: 10.1063/1.5035085

Abstract

Resistivity of metastable amorphous Ge2Sb2Te5 (GST) measured at device level show an exponential decline with temperature matching with the steady-state thin-film resistivity measured at 858 K (melting temperature). This suggests that the free carrier activation mechanisms form a continuum in a large temperature scale (300 K – 858 K) and the metastable amorphous phase can be treated as a super-cooled liquid. The effective activation energy calculated using the resistivity versus temperature data follow a parabolic behavior, with a room temperature value of 333 meV, peaking to ∼377 meV at ∼465 K and reaching zero at ∼930 K, using a reference activation energy of 111 meV (3kBT/2) at melt. Amorphous GST is expected to behave as a p-type semiconductor at Tmelt ∼ 858 K and transitions from the semiconducting-liquid phase to the metallic-liquid phase at ∼ 930 K at equilibrium. The simultaneous Seebeck (S) and resistivity versus temperature measurements of amorphous-fcc mixed-phase GST thin-films show linear S-T...

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