2003
DOI: 10.1134/1.1579818
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Deterministic noise in vanadium dioxide based structures

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Cited by 14 publications
(16 citation statements)
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“…Chaotic oscillations have been obviously first observed in [7]. The experimental works have been carried out on single crystals [5,8], thin films [6], [9], [10] and ceramics [7]. Chaotic dynamics and noise effects in vanadium dioxide are of considerable interest because of potential technical applications of the material.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Chaotic oscillations have been obviously first observed in [7]. The experimental works have been carried out on single crystals [5,8], thin films [6], [9], [10] and ceramics [7]. Chaotic dynamics and noise effects in vanadium dioxide are of considerable interest because of potential technical applications of the material.…”
Section: Introductionmentioning
confidence: 99%
“…Chaotic dynamics and noise effects in vanadium dioxide are of considerable interest because of potential technical applications of the material. In addition, these effects receive increased attention due to general fundamental interest both in the nonlinear phenomena themselves, and, in particular, in the problem of metal-insulator transitions, because the noise measurements can give valuable information about the transition mechanism [4][5][6], [8], [10]. As for the applied aspect, vanadium oxide films are used for fabrication of a variety of electrical and optical devices, including electrical switching elements, temperature sensors, optical storage devices, variable reflectivity mirrors, IR bolometric detectors [11].…”
Section: Introductionmentioning
confidence: 99%
“…The frequency scatter of about 2% is associated with a general instability of the threshold voltage described in Ref. .…”
Section: Resultsmentioning
confidence: 94%
“…The current ID1 is varied in the NDR range, from Ih to Ith (0.4 -1 mA), with the steps of 10 μA, though the stable self-oscillation generation is observed not in the entire range, but only within the ID1 values from about 590 to 880 μA. This is due to the fact that, as the operating point approaches the I-V curve thresholds (ID1 → Ih, Ith), the internal noise [22] starts to play an important role and the oscillations transit from a steady state to a burst mode [23]. The dependence of the oscillation frequency F 0 1 on the supply current ID1 is practically linear (Fig.…”
Section: Resultsmentioning
confidence: 99%