1997
DOI: 10.1016/s0169-4332(97)80114-6
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The properties of Schottky junctions on Nb-doped SrTiO3 (001)

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Cited by 66 publications
(43 citation statements)
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“…For the interface between the gold AFM tip and the SrTiO 3 , which consists of an uncontrolled and unknown interface, Φ eff = 1.3 eV and n = 1.3. These properties are in the same range as those reported earlier [14]- [18] In the cases of the macroscopic electrodes and the AFM tip-substrate contact, the structure of the interface is random. The more controlled interfaces will allow properties to be related to interface structure and size.…”
Section: B Fabrication and Testingsupporting
confidence: 83%
“…For the interface between the gold AFM tip and the SrTiO 3 , which consists of an uncontrolled and unknown interface, Φ eff = 1.3 eV and n = 1.3. These properties are in the same range as those reported earlier [14]- [18] In the cases of the macroscopic electrodes and the AFM tip-substrate contact, the structure of the interface is random. The more controlled interfaces will allow properties to be related to interface structure and size.…”
Section: B Fabrication and Testingsupporting
confidence: 83%
“…Shimuzu et al have measured the SBHs from various metal/SrTiO 3 junctions and plotted the SBHs as a function of Pauling's electronegativity of the metals. They show that the determined slope parameter S X is about 1, which suggests that the interfacial electronic states are not dominant in the interface charge transfer process at metal/SrTiO 3 interfaces (see discussion in Section 2.1.1) [438].…”
Section: Metal-srtio 3 Interactionsmentioning
confidence: 97%
“…The reported data, however, are scattered since the sample preparation condition are quite different among the authors. For example, Shimizu et al pretreated single crystals of Nb-SrTiO 3 by chemical etching and the succeeding ozone cleaning at elevated temperatures, and reported that the barrier was well explained by the Schottky limit [2]. The ozone treatment makes the surface of the sample in a highly oxidized state.…”
Section: Sensitivity To Oxygenmentioning
confidence: 99%
“…E-mail: kawada@tagen.tohoku.ac.jp clarified enough. For donor doped SrTiO 3 , the grain boundary or the surface are known to have much higher resistance than the bulk [1][2][3][4][5][6][7][8][9]. Niobium segregation, Sr vacancy and/or Sr n+1 Ti n O 3n+1 phase formation, or Schottky barrier have been considered in the literatures as the reason of the high resistivity.…”
Section: Introductionmentioning
confidence: 99%