Figure 7
Thermal magnetoresistance: The thermal magnetoresistance (MR) as a function of T L with different ΔT (a–c) and ΔT with different T L (d–f) by changing the heterojunction from ground state to magnetic states, that is, (a) and (d) [AFM-AFM] → [AFM-FM], (b) and (e) [AFM-AFM] → [FM-AFM], (c) and (f) [AFM-AFM] → [FM-FM]. The inset of (a) is a magnified view and the inset of (c) is the net electron charge currents I C versus T L for ΔT = 20 K, 40 K and 60 K in the ground state.
