Here, we suppose the identical energy dissipation of one cell in different RESET processes. The integration energy curve agrees well with the experimental fitting curve as shown in Figure 4d. The energy decays exponentially during the RESET with the elevated environmental temperature. Therefore, when charge detrapping dependence

on environmental temperature is involved as in Equation 1, the calculated mean value of energy consumption in RESET decreased exponentially, which in good agreement with experimental results in Figure 4d. Although the switching parameters such as SET voltage, RESET current, and resistance of LRS or HRS vary with cycles, Mocetinostat mw the statistical energy consumption still decays exponentially with the elevated environmental temperature when involving the charge trapping effect at low temperature. Figure 4 Statistical distribution of device parameters and the calculated correlation between the energy versus sample temperature. (a) LRS resistance (measured at 0.3 V), (b) RESET voltage, and (c) RESET current statistics at different temperatures. (d) Statistics on energy consumption during the RESET process as calculated.

Here, the small square in the middle of the large square is the average mean value of the device parameters, and the large square indicates the distribution factors of 75% (top line) and 25% (bottom line), respectively. click here The black solid line in (d) is the average value line, and the red line is the statistical value fit

line. Figure 5 is the experimental I V data of HRS at different temperatures and the fitting curves by hopping and Frenkel-Poole conduction mechanism, respectively. The electron conduction in HRS of NbAlO at 80 to 130 K as shown in Figure 5a can be fitted well with hopping model because of the characteristic temperature dependence. A linear relationship between ln(I/V) vs. V 1/2 can be obtained at 130 to 180 K as shown in Figure 5b. It indicates that the I V relation obeys the Frenkel-Poole conduction mechanism with the expression as in the equation below: where I is the current, q is the electron charge, V is the applied voltage, α is a constant, b is the energy barrier height, k is Boltzmann’s constant, and T is the temperature in Kelvin. Therefore, the transition temperature of 130 K from variable Sclareol hopping conduction to Frenkel-Poole conduction for NbAlO HRS is confirmed and attracts research attention. It is believed that the density of trapped electrons or the local states in the oxide film play an important role as previous report described [15, 16]. The temperature transition region should be different for different materials because of the local states and defect density differences. Figure 5 Experimental I – V data of HRS at different temperatures. (a) Linear fitting for the I-V curve at higher temperatures (80 to 130 K) using a log-log scale.