2014
DOI: 10.1016/j.microrel.2013.10.013
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Oxygen vacancy formation and the induced defect states in HfO2 and Hf-silicates – A first principles hybrid functional study

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Cited by 8 publications
(6 citation statements)
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“…[43,1,33] Upon annealing at temperatures above 400 -600 • C, dependant upon growth technique and substrate, the degree of crystalline character increases forming cubic and or monoclinic crystalline regions within the film, which at elevated temperatures > 900 • C give the completely poly-crystalline thin film. [6,72,30] The picture given by the XRD peaks is further confirmed when the partially crystalline and poly-crystalline films are studied using TEM, showing crystal like islands at the low end of the temperature scale. These structures expand as temperature is increased resulting in the high temperature poly-crystalline films.…”
Section: Introductionmentioning
confidence: 62%
“…[43,1,33] Upon annealing at temperatures above 400 -600 • C, dependant upon growth technique and substrate, the degree of crystalline character increases forming cubic and or monoclinic crystalline regions within the film, which at elevated temperatures > 900 • C give the completely poly-crystalline thin film. [6,72,30] The picture given by the XRD peaks is further confirmed when the partially crystalline and poly-crystalline films are studied using TEM, showing crystal like islands at the low end of the temperature scale. These structures expand as temperature is increased resulting in the high temperature poly-crystalline films.…”
Section: Introductionmentioning
confidence: 62%
“…the HfOx layer owing to the presence of oxygen vacancies in the HfOx. [60][61][62][63] Nevertheless, HfOx is able to accept oxygen only to some extent. Oxygen anions not able to enter the HfOx lattice are involved in the oxidation of a fraction of CoO to Co3O4 (Figure 8e).…”
Section: Resultsmentioning
confidence: 99%
“…More specifically, as depicted in Figure d,e, the application of negative voltage to the Co–Pt/HfO x system triggers the diffusion of O 2– ions from the Co–Pt film toward the HfO x layer, resulting in the partial reduction of Co 3 O 4 to CoO and the reduction of CoO to metallic Co. Unlike the uncoated Co–Pt films, for which O 2– migration was limited to the surface, oxygen ions can diffuse here within the HfO x layer owing to the occurrence of oxygen vacancies in HfO x . Nevertheless, HfO x is able to accept oxygen only to some extent. Oxygen anions not able to enter the HfO x lattice are involved in the oxidation of a fraction of CoO to Co 3 O 4 (Figure e).…”
Section: Resultsmentioning
confidence: 99%
“…5(b), which is agreed with the trapping energy of V o in α-HfO x . [34] The conduction in the LRS could thus be governed by a Poole-Frenkel emission mechanism with the V o s assisting electron transport in the HfO x .…”
Section: Switching Mechanism Of the Rramsmentioning
confidence: 99%