2010
DOI: 10.1063/1.3435466
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Nanoscale imaging and control of resistance switching in VO2 at room temperature

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Cited by 127 publications
(100 citation statements)
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References 20 publications
(15 reference statements)
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“…37,57,58 Depending on the film quality, the conductivity increases by 3 -4 orders of magnitude when heating the samples above the MIT temperature. Adopting a resistivity of 1 cm for VO 2 at room temperature and 1 m cm at …”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…37,57,58 Depending on the film quality, the conductivity increases by 3 -4 orders of magnitude when heating the samples above the MIT temperature. Adopting a resistivity of 1 cm for VO 2 at room temperature and 1 m cm at …”
Section: Resultsmentioning
confidence: 99%
“…[27][28][29][30][31][32][33][34][35][36][37][38][39] An interesting MIT system as candidate to generate conducting ion tracks or generally to produce ion-induced conductivity changes is VO 2 . VO 2 exhibits a reversible temperature driven MIT, which markedly changes its electronic and optical properties.…”
mentioning
confidence: 99%
“…25,26 These filaments were interpreted as electrical instabilities related to the peculiar S-shaped I-V characteristics measured in VO 2 , in particular to their region of negative differential resistance (NDR). [27][28][29][30] Only a comprehensive microscopic theory of RS in correlated insulators, compatible with all the experimental evidence at hand, can resolve this long-standing puzzle. The recently proposed classical resistor network models 1,2,20,31-34 successfully reproduced part of the phenomenology but these are heuristic approaches, not firmly grounded from a microscopic perspective.…”
mentioning
confidence: 99%
“…Vanadium dioxide (VO 2 ) is well known as a typical material invoking an electronic phase transition between a high-temperature metallic state and a low-temperature insulating state accompanied by orders of magnitude changes in resistance at 340 K. 7,8 In the vicinity of the metal-insulator transition (MIT) temperature, VO 2 has mixed electronic phases consisting of metal and insulator domains, 3,9 obscuring the intrinsic properties of the phase transition. By reducing the sample size to a single domain, on the other hand, a steep first-order phase transition for individual domains can be observed.…”
Section: Introductionmentioning
confidence: 99%
“…[10][11][12] Regarding the characteristics of the phase transition, ultra-fast 13 and spatial avalanche transitions in domains 10,14,15 have been reported. Thus, electronic control of the transition in the two terminal devices has much attracted attention; 9,[16][17][18][19] however, the control enables only a one-way transition, from insulator to metal (I-to-M). Inherently, the transition using an electric bias is caused by Joule heating, 19,20 which is unlikely to present reversible controllability of the transition.…”
Section: Introductionmentioning
confidence: 99%