Recently, the mechanism of resistive random access memory (RRAM) has been partly clarified and determined to be controlled by the forming and erasing of conducting filaments (CF). However, the size of the CF may restrict the application and development as devices are scaled down. In this work, we synthesized CuO nanowires (NW) ($150 nm in diameter) to fabricate a CuO NW RRAM nanodevice that was much smaller than the filament ($2 lm) observed in a bulk CuO RRAM device in a previous study. HRTEM indicated that the Cu 2 O phase was generated after operation, which demonstrated that the filament could be minimize to as small as 3.8 nm when the device is scaled down. In addition, energy dispersive spectroscopy (EDS) and electron energy loss spectroscopy (EELS) show the resistive switching of the dielectric layer resulted from the aggregated oxygen vacancies, which also match with the I-V fitting results. Those results not only verify the switching mechanism of CuO RRAM but also show RRAM has the potential to shrink in size, which will be beneficial to the practical application of RRAM devices. V C 2015 AIP Publishing LLC.Conventional charge-based flash memories, such as floating-gate nonvolatile flash memory, are rapidly approaching their physical limits. 1 To satisfy numerous data computing and storage applications, non-volatile memory (NVM) has attracted significant interest for extensive studies in recent years. This type of memory consists of phase change random access memory (PCRAM), magnetic RAM (MRAM), and resistive RAM (RRAM). Among them, RRAM is the most powerful candidate because of its excellent endurance, retention, low power consumption, fast write/speed read, and simple metal/insulator/metal (MIM) structure. 2 To improve the RRAM performance, a complete understanding of its switching properties is necessary. Recently, the mechanism of resistive switching behavior has been partly clarified and determined that it relies on the generation of a conducting filament. When one of the electrodes is an active metal, such as Ag or Cu, the active metal will be oxidized into ions and the electrical field will then drive metal ions into the dielectric layer. The conducting filaments (CF) will be generated from the reduction of metal ions, called electro-chemical metallization (ECM). 3 On the other hand, when both electrodes are inert metals, such as Au or Pt, the anion migration in the insulator will lead to resistive switching. 4 The conducting filament will be composed of oxygen vacancies, called the valence change mechanism (VCM), 3 although the mechanism is still unclear in many dielectric layers.These different type of conducting filaments have been observed in recent years; for example, the real time observation of the Zn structure filament in the ZnO dielectric layer 5 and the Ti 4 O 7 filament of in the TiO 2 layer 6 in a VCM system. The active metal type filament can generate a conducting bridge in various dielectric layers in an ECM system. [7][8][9][10][11] By controlling the formation and rupture of the f...