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https://doi.org/10.1063/1.3460108
DC Field | Value | |
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dc.title | ZnO as a buffer layer for growth of BiFeO3 thin films | |
dc.contributor.author | Wu, J. | |
dc.contributor.author | Wang, J. | |
dc.date.accessioned | 2014-10-07T09:55:34Z | |
dc.date.available | 2014-10-07T09:55:34Z | |
dc.date.issued | 2010-08-01 | |
dc.identifier.citation | Wu, J., Wang, J. (2010-08-01). ZnO as a buffer layer for growth of BiFeO3 thin films. Journal of Applied Physics 108 (3) : -. ScholarBank@NUS Repository. https://doi.org/10.1063/1.3460108 | |
dc.identifier.issn | 00218979 | |
dc.identifier.uri | http://scholarbank.nus.edu.sg/handle/10635/86851 | |
dc.description.abstract | Multiferroic BiFeO3 thin film was grown on the ZnO-buffered Pt/TiO2/SiO2/Si (100) substrate by off-axis radio frequency magnetron sputtering, where the ZnO buffer layer gave rise to a strong (110) texture for the BiFeO3 thin film. The resulting BiFeO 3/ZnO thin film exhibits diode-like and resistive hysteresis behavior, in which the resistive hysteresis and rectifying ratio are dependent on the applied voltage and temperature. The resistive switching behavior of the BiFeO3 /ZnO thin film is shown to relate to the trap-controlled space charge limited conduction and interface-limited Fowler-Nordheim tunneling, while the polarization reversal takes place in the BiFeO3 layer of the heterostructure. The BiFeO3 /ZnO thin film is also demonstrated with a higher remanent polarization (2 Pr ∼ 153.6 μC/cm 2), a much lower dielectric loss (tan δ∼0.012), and a better fatigue endurance as compared to those of the BiFeO3 thin film without a ZnO buffer layer, where the much reduced leakage is largely responsible for the enhanced ferroelectric behavior. The ZnO as a buffer layer for BiFeO3 significantly changes the dielectric relaxation and conduction mechanisms, when the dielectric relaxation and electrical conduction are governed by the thermal excitation of carriers from the second-ionization and short-range motion of oxygen vacancies, respectively, while the relaxation process remains the same over the entire temperature range of 20 to 200 °C investigated in the present study. © 2010 American Institute of Physics. | |
dc.description.uri | http://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1063/1.3460108 | |
dc.source | Scopus | |
dc.type | Article | |
dc.contributor.department | MATERIALS SCIENCE AND ENGINEERING | |
dc.description.doi | 10.1063/1.3460108 | |
dc.description.sourcetitle | Journal of Applied Physics | |
dc.description.volume | 108 | |
dc.description.issue | 3 | |
dc.description.page | - | |
dc.description.coden | JAPIA | |
dc.identifier.isiut | 000280941000083 | |
Appears in Collections: | Staff Publications |
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