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Field and polarity dependence of time-to-resistance increase in Fe–O films studied by constant voltage stress method
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10.1063/1.3064127
/content/aip/journal/apl/94/1/10.1063/1.3064127
http://aip.metastore.ingenta.com/content/aip/journal/apl/94/1/10.1063/1.3064127
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Current vs voltage characteristics for Fe–O films. The vertical axis on the left is an initial current (: dotted lines) and that on the right is the current for various resistance-changed devices (: solid lines). Example for the resistance change process is shown in the inset.

Image of FIG. 2.
FIG. 2.

Examples of time evolution of injected current under a constant voltage stress [] for various stress conditions with different polarities. Time-to-resistance change is judged as the change in , respectively.

Image of FIG. 3.
FIG. 3.

Time-to-resistance increase as a function of stress voltage for various stress conditions with different polarities (positive stress: open circle, negative stress: closed circle.) The for Fe–O multilayer structure is also shown for comparison. (positive stress: open triangle, negative stress: closed triangle.)

Image of FIG. 4.
FIG. 4.

Cumulative probabilities of a critical voltage for the resistance change with different stress polarities.

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/content/aip/journal/apl/94/1/10.1063/1.3064127
2009-01-08
2014-04-24
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Field and polarity dependence of time-to-resistance increase in Fe–O films studied by constant voltage stress method
http://aip.metastore.ingenta.com/content/aip/journal/apl/94/1/10.1063/1.3064127
10.1063/1.3064127
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