An
emerging nonvolatile, solid-state memory is resistance random
access memory (RRAM). RRAM is based on reversible switching of resistance
in semiconductor and insulator thin films. Here, unipolar resistance
switching is demonstrated in electrodeposited films of [111]-textured
cuprous oxide (Cu<sub>2</sub>O). The textured Cu<sub>2</sub>O is electrodeposited
from a highly alkaline bath using tartrate as the complexing agent.
The switching is observed in a cell composed of a film of Cu<sub>2</sub>O sandwiched between Au and Au–Pd contacts. The switching
is attributed to the formation and rupture of a Cu nanofilament in
the Cu<sub>2</sub>O. The initial resistance of the cell is 6.5 ×
10<sup>6</sup> Ω, and a conducting filament is formed in the
film by scanning the applied electric field to 6.8 × 10<sup>6</sup> V m<sup>–1</sup>. The cell is then reversibly cycled between
a low resistance state of 16.6 Ω and a high resistance state
of 4 × 10<sup>5</sup> Ω by the SET and RESET processes.
In the low resistance state, the resistance decreases linearly with
decreasing temperature, consistent with metallic behavior. The resistance
temperature coefficient of 1.57 × 10<sup>–3</sup> K<sup>–1</sup> is similar to that of nanoscale metallic Cu. Current–voltage
(<i>I</i>–<i>V</i>) data suggests that
applying a higher compliance current increases the filament size during
the FORMING and the SET process and also causes a higher RESET current.
The filament diameter varies from 50 to 147 nm for compliance currents
ranging from 10 to 100 mA. At high electric field in the as-deposited
state, the conduction behavior follows Poole-Frenkel emission. The
filament temperature is estimated from the nonohmic behavior of the
cell in the RESET step. The calculated temperature of 798 K before
rupture of the Cu filament suggests Joule heating of the filament,
resulting in melting, sintering, or thermal oxidation of the Cu filament