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The existence of reversible resistance switching (RS) behaviors induced by electric stimulus has been known for some time, [1][2][3] and these intriguing physical phenomena have been observed in numerous materials, including oxides. [4][5][6][7][8][9][10][11][12][13][14][15][16][17] As conventional charge-based random access memory is expected to face a size limit in the near future, a surge of renewed interest has been developed in RS phenomena for possible applications in small nonvolatile memory devices called resistance random access memory (RRAM).Of particular interest is unipolar RS, which shows the RS at two values of applied voltage of the same polarity. [15][16][17] The unipolar RS exhibits a much larger resistance change than other RS phenomena, and this greatly simplifies the process of reading the memory state.
The existence of reversible resistance switching (RS) behaviors induced by electric stimulus has been known for some time, [1][2][3] and these intriguing physical phenomena have been observed in numerous materials, including oxides. [4][5][6][7][8][9][10][11][12][13][14][15][16][17] As conventional charge-based random access memory is expected to face a size limit in the near future, a surge of renewed interest has been developed in RS phenomena for possible applications in small nonvolatile memory devices called resistance random access memory (RRAM).Of particular interest is unipolar RS, which shows the RS at two values of applied voltage of the same polarity. [15][16][17] The unipolar RS exhibits a much larger resistance change than other RS phenomena, and this greatly simplifies the process of reading the memory state.