2006
DOI: 10.1063/1.2236213
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Spatially extended nature of resistive switching in perovskite oxide thin films

Abstract: We report the direct observation of the electric pulse induced resistancechange (EPIR) effect at the nano scale on La 1-x Sr x MnO 3 (LSMO) thin films by the current measurement AFM technique. After a switching voltage of one polarity is applied across the sample by the AFM tip, the conductivity in a local nanometer region around the AFM tip is increased, and after a switching voltage of the opposite polarity is applied, the local conductivity is reduced. This reversible resistance switching effect is observed… Show more

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Cited by 97 publications
(66 citation statements)
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“…A simplified memristor device physics model [1] matched the experimental behavior [2] of nanocrossbar Pt/TiO 2 /Pt devices. Resistive switching in metal oxides has in fact seen more than four decades of scientific research [4][5][6][7][8][9][10][11][12][13][14][15], motivated in large part by that prospect of a fast and high density NVRAM technology [16][17][18][19][20][21][22][23]. The continuous resistance change exhibited by oxide switches also appears to meet analog switch requirements for neuromorphic computing [24][25][26].…”
Section: Introductionmentioning
confidence: 99%
“…A simplified memristor device physics model [1] matched the experimental behavior [2] of nanocrossbar Pt/TiO 2 /Pt devices. Resistive switching in metal oxides has in fact seen more than four decades of scientific research [4][5][6][7][8][9][10][11][12][13][14][15], motivated in large part by that prospect of a fast and high density NVRAM technology [16][17][18][19][20][21][22][23]. The continuous resistance change exhibited by oxide switches also appears to meet analog switch requirements for neuromorphic computing [24][25][26].…”
Section: Introductionmentioning
confidence: 99%
“…Resistive switching has been commonly observed in various oxides, e.g., Cu x O, 1 NiO, 2,3 TiO 2 , 4-6 SrTiO 3 , 7-9 BaTiO 3 , 10 ͑Ba, Sr͒TiO 3 , 11 SrZrO 3 , 12 La 1−x Sr x MnO 3 , 13 and Pr 1−x Ca x MnO 3 , [14][15][16] as well as in higher chalcogenides, e.g., Ag or Cu doped Ge x Se 1−x , 17,18 Ag 2 S, 19 and Cu 2 S. 20 Quite diverse switching mechanisms have been proposed, based on thermal, electronic, and/or electrochemical effects. In particular, when one involved electrode metal is situated in the intermediate range of the electrochemical potential series and forms mobile cations, such as Ag + and Cu + , bipolar switching characteristics are observed, and electrochemical redox processes are generally accepted to be responsible for the switching.…”
mentioning
confidence: 99%
“…[10][11][12][13][14] At a threshold voltage called the traps-filled-limit voltage, current flow undergoes a sharp transition from a relatively high-resistance Ohm's law regime to a low-resistance Mott-Gurney's law regime as manifested by a steep rise in current. Resistance switching in metal/oxide/metal devices has been observed and attributed to interface 15 or bulk 16,17 charge-induced changes in the interface barrier height. Capacitance-voltage measurements indicate that there is no insulating layer at the n-GaAs / semi-insulating GaAs substrate interface.…”
Section: Copyright 2012 Author(s) This Article Is Distributed Under mentioning
confidence: 99%