Figure 6

Schematics of the Resistive Switching Mechanism: Schematic showing the drift of boron ions (B−, solid balls) towards the Pt tip at high positive bias. At low bias, B− ions diffuse back to annihilate the boron vacancy (open circles), reducing the overall conductivity of the h-BN/Cu stack. The directional movement of B− ions is governed by the interplay between diffusion and drift. The length of arrows indicates qualitatively the relative magnitude of drift and diffusion flux of B− ions.