Understanding the Resistive Switching Phenomena of Stacked Al/Al<sub>2</sub>O<sub>3</sub>/Al Thin Films from the Dynamics of Conductive Filaments

<div><svg height="8.98583pt" id="M19" style="vertical-align:-0.3499308pt" version="1.1" viewbox="-0.0498162 -8.6359 28.4066 8.98583" width="28.4066pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><g transform="matrix(.013,0,0,-0.013,0,0)"><path d="M405 650H141L135 622C222 616 230 610 215 535L133 116C118 41 113 33 29 28L23 0H289L295 28C209 33 205 40 219 116L298 535C312 609 317 616 399 622L405 650Z" id="g113-74"></path></g><g transform="matrix(.013,0,0,-0.013,8.473,0)"><path d="M535 230V280H52V230H535Z" id="g117-33"></path></g><g transform="matrix(.013,0,0,-0.013,19.009,0)"><path d="M697 650H468L461 623L492 619C539 613 547 605 518 546C481 471 367 264 278 116H276C239 278 197 500 186 567C180 604 185 613 226 619L252 623L260 650H24L17 623C78 617 92 613 108 533L216 -11H247C365 200 515 462 560 529C616 612 624 615 689 623L697 650Z" id="g113-87"></path></g></svg> diagrams showing the (a) unipolar and (b) bipolar operation modes for ReRAM devices where no dependence of the<i> “pinched hysteresis loops”</i> to frequency is involved (DC conditions). 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Complexity

fig1

Figure 1

Figure 1: Understanding the Resistive Switching Phenomena of Stacked Al/Al<sub>2</sub>O<sub>3</sub>/Al Thin Films from the Dynamics of Conductive Filaments 

Complexity

Understanding the Resistive Switching Phenomena of Stacked Al/Al2O3/Al Thin Films from the Dynamics of Conductive Filaments

Figure 1

Understanding the Resistive Switching Phenomena of Stacked Al/Al₂O₃/Al Thin Films from the Dynamics of Conductive Filaments