001     50923
005     20190625110508.0
024 7 _ |2 pmid
|a pmid:16565712
024 7 _ |2 DOI
|a 10.1038/nmat1614
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|a WOS:000236530400023
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037 _ _ |a PreJuSER-50923
041 _ _ |a eng
082 _ _ |a 610
084 _ _ |2 WoS
|a Chemistry, Physical
084 _ _ |2 WoS
|a Materials Science, Multidisciplinary
084 _ _ |2 WoS
|a Physics, Applied
084 _ _ |2 WoS
|a Physics, Condensed Matter
100 1 _ |a Szot, K.
|b 0
|u FZJ
|0 P:(DE-Juel1)VDB2799
245 _ _ |a Switching the electrical resistance of individual dislocations in single-crystalline SrTiO3
260 _ _ |a Basingstoke
|b Nature Publishing Group
|c 2006
300 _ _ |a 312
336 7 _ |a Journal Article
|0 PUB:(DE-HGF)16
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336 7 _ |a article
|2 DRIVER
440 _ 0 |a Nature Materials
|x 1476-1122
|0 11903
|y 4
|v 5
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a The great variability in the electrical properties of multinary oxide materials, ranging from insulating, through semiconducting to metallic behaviour, has given rise to the idea of modulating the electronic properties on a nanometre scale for high-density electronic memory devices. A particularly promising aspect seems to be the ability of perovskites to provide bistable switching of the conductance between non-metallic and metallic behaviour by the application of an appropriate electric field. Here we demonstrate that the switching behaviour is an intrinsic feature of naturally occurring dislocations in single crystals of a prototypical ternary oxide, SrTiO(3). The phenomenon is shown to originate from local modulations of the oxygen content and to be related to the self-doping capability of the early transition metal oxides. Our results show that extended defects, such as dislocations, can act as bistable nanowires and hold technological promise for terabit memory devices.
536 _ _ |a Kondensierte Materie
|c P54
|2 G:(DE-HGF)
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588 _ _ |a Dataset connected to Web of Science, Pubmed
650 _ 2 |2 MeSH
|a Aluminum Oxide: chemistry
650 _ 2 |2 MeSH
|a Crystallization
650 _ 2 |2 MeSH
|a Electric Conductivity
650 _ 2 |2 MeSH
|a Electric Impedance
650 _ 2 |2 MeSH
|a Electromagnetic Fields
650 _ 2 |2 MeSH
|a Electronics
650 _ 2 |2 MeSH
|a Metals: chemistry
650 _ 2 |2 MeSH
|a Microscopy, Atomic Force
650 _ 2 |2 MeSH
|a Nanotechnology: methods
650 _ 2 |2 MeSH
|a Oxides: chemistry
650 _ 2 |2 MeSH
|a Oxygen: chemistry
650 _ 2 |2 MeSH
|a Strontium: chemistry
650 _ 2 |2 MeSH
|a Surface Properties
650 _ 2 |2 MeSH
|a Temperature
650 _ 2 |2 MeSH
|a Titanium: chemistry
650 _ 7 |0 0
|2 NLM Chemicals
|a Metals
650 _ 7 |0 0
|2 NLM Chemicals
|a Oxides
650 _ 7 |0 12060-59-2
|2 NLM Chemicals
|a strontium titanium oxide
650 _ 7 |0 1344-28-1
|2 NLM Chemicals
|a Aluminum Oxide
650 _ 7 |0 7440-24-6
|2 NLM Chemicals
|a Strontium
650 _ 7 |0 7440-32-6
|2 NLM Chemicals
|a Titanium
650 _ 7 |0 7782-44-7
|2 NLM Chemicals
|a Oxygen
650 _ 7 |a J
|2 WoSType
700 1 _ |a Speier, W.
|b 1
|u FZJ
|0 P:(DE-Juel1)125382
700 1 _ |a Bihlmayer, G.
|b 2
|u FZJ
|0 P:(DE-Juel1)130545
700 1 _ |a Waser, R.
|b 3
|u FZJ
|0 P:(DE-Juel1)131022
773 _ _ |a 10.1038/nmat1614
|g Vol. 5, p. 312
|p 312
|q 5<312
|0 PERI:(DE-600)2088679-2
|t Nature materials
|v 5
|y 2006
|x 1476-1122
856 7 _ |u http://dx.doi.org/10.1038/nmat1614
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