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Preparation And Multiferroics Properties Research Of BiFeO3 Nanoceramics

Posted on:2019-12-09Degree:DoctorType:Dissertation
Country:ChinaCandidate:Y H TianFull Text:PDF
GTID:1361330545490376Subject:Microelectronics and Solid State Electronics
Abstract/Summary:PDF Full Text Request
Multiferroic materials are a class of materials of processing two or more ferroic ordering,such as ferroelectric,ferromagnetic,and ferroelasticity.Meanwhile these ferroic ordering can couple with each other.BiFeO3 is a well known room temperature multiferroic material with ferroelectric ordering below 1103 K and G-type antiferromagnetic ordering below 643 K,which offered a wide range of potential applications such as multi-states storage,and non-volatile magnetoelectric memory.Based on this situation,we have prepared BiFeO3 nanoceramics by spark plasmas sintering method,and improved its magnetic properties by breaking the antiparallel spin with helical repeat of?62 nm.Dielectric properties,magnetic properties,and defects types were investigated in BiFeO3 ceramics with different grains size.On the basis of the abovementioned research,the properties of ferroelectric,dielectric,and ferromagnetic were investigated in Ti doped BiFeO3 nanoceramics(BiFe0.95Ti0.05O3).The influence of grain size and structural distortion on multiferroic properties of Ti doped BiFeO3nanoceramics were analysied.Further,we compared the ferroelectric and magnetic properties of different lanthanide(Gd3+and Ho3+)doped BiFe0.95Ti0.05O3 nanoceramics samples.The results are shown as follows:1.The study of grain-size-effect and preparing of BiFeO3 nanoceramics.Single-phased BiFeO3 nanoceramics were obtained by spark plasmas sinering method.Medium-grained?grain size=500 nm?and coarser-grained?grain size=1.2?m?BiFeO3ceramics were prepared for comparison using the same method.The XRD patterns demonstrated that all samples contained a single phase without other phases.The effects of grain size on the electric and ferromagnetism of pure phase BiFeO3 ceramics were investigated.The results indicated that the decreasing grain size helped to decrease the content of Fe2+ions and dielectric loss in BiFeO3 samples.Thus the dielectric properties in BiFeO3 nanoceramics have been improved..For the meauremnt of ferromagnetic properties,BiFeO3 nanoceramics?S1?possess a good performance of ferromagnetic?Mr=0.01 emu/g?,which was much larger than the coarser-grained BiFeO3 ceramics?Mr=0.0057 emu/g?.This phenomenon can be explained as the broken of spin spiral structure with the decrease of grain size.A large value of exchange bias(HEB=500 Oe)was observed for S1 samples at 5 K,which can be explained as an exchange interaction between the small grains?below 62 nm?with ferromagnetic state and the big grains?above62nm?withantiferromagneticstate.Themeasurementof magnezation-temperature indicated the existence of spin glass state in BiFeO3nanoceramics.2.Preparing of BiFe0.95Ti0.05O3 nanoceramics and their properties improved by Ti doping.Based on the study of phase pure BiFeO3 nanoceramics,a strategy of doping Ti4+ion at B-site was adoped,to promote the property of multiferroic in BiFeO3 based ceramics.Many test methods have been carried in Ti-doped BiFeO3 nanoceramics to study their microstructure,ferroelectric and ferromagnetic properties.Ti-doped BiFeO3nanoceramics with an average grain size less than 100 nm exhibited a rhombohedral phase.Comparing to the single phase BiFeO3 nanoceramics,the dielectric loss of BiFe0.95Ti0.05O3was remarkably reduced?tan?=0.02?.For the measurement of impedance spectrum,the valence fluctuation of Fe ions in BiFe0.95Ti0.05O3 nanoceramics was significantly supressed,and the diffusion of oxygen ion was the major reason for dielectric relaxation at high temperature.The remenant polarization and P-E loops confirmed the intrinsic ferroelectric in BiFe0.95Ti0.05O3 nanoceramcis.The PFM measurements showed nanoscaled ferroelectric domains for BiFe0.95Ti0.05O3 nanoceramics.Those results demonstrated the exisintance of ferroelectric properties in BiFe0.95Ti0.05O3 nanoceramics.Meanwhile,high remnant magnetization?Mr=0.1 emu/g,Ms=0.5 emu/g?were observed.Comparing to the results of BiFeO3 nanoceramics,the ferroelectric and ferromagnetic properties were significant improved in BiFe0.95Ti0.05O3 nanoceramics with a rhombohedral phase.3.Preparing of Bi0.8Gd0.2Fe1-xTixO3 nanoceramics and their properties improved by Gd3+and Ti4+doping.The prior studied BiFeO3 system was mainly rhombohedral phase,to further improve the ferromagnetic properties,a change in crystal structure was necessary.Results show that Ln3+doping at A-sites could introduce a orthorhombic structure in BiFeO3 system.An increase in the induced magnetic moment was caused by the structure evolution.Hence,to obtain orthorhombic phase with good magnetic property,Bi0.8Gd0.2Fe1-xTixO3?x=0,0.03,0.05?nanoceramcis were prepared by spark plasma sintering method,and their structure,ferroelectric and ferromagnetic behaviors were investigated.Bi0.8Gd0.2Fe0.97Ti0.03O3 and Bi0.8Gd0.2Fe0.95Ti0.05 samples showed a mixture structure with three kinds of space group?R3c,Pnma,and Pn21a?.And there were two kinds of space group?R3c and Pnma?in Bi0.8Gd0.2FeO3 samples.Relaxor ferroelectric-paraelectric transition peaks were observed.The relaxor behavior in BGFO ceramics comes from the disorder distributions of Bi3+and Gd3+(or Fe2+and Fe3+)ions on the crystallographically equivalent sites.The ferroelectric measurement of Bi0.8Gd0.2Fe0.97Ti0.03O3 and Bi0.8Gd0.2Fe0.95Ti0.05 samples showed an obvious ferroelectric polarization owing to a low leakage current density.For the measurement of ferromagnetic properties,the improved magnetism in Bi0.8Gd0.2Fe1-xTixO3 nanoceramics?Ms?1.0emu/g?can be explained as:?a?The increase in the induced magnetic moment caused by the structure evolution;?b?the broken of the antiparallel spin.This paper has verified the existence of good multiferroic properties in co-doped samples.4.Preparing of orthorhombic structure Bi0.8Ho0.2Fe0.95Ti0.05O3 nanoceramics and their magnetic properties improved with Ho3+and Ti4+doping.The previous section has described the structure and multiferroic properties in Bi0.8Gd0.2Fe1-xTixO3 nanoceramics.As a comparison,we selected smaller ion radius Ho3+,the properties of ferroelectric and ferromagnetic in Bi0.8Ho0.2Fe0.95Ti0.05O3 nanoceramics were studied.Ho3+has higer magnetic moment for larger number of 4f electrons than Gd3+,and Ho3+doped BiFeO3 has larger crystal distortion for smaller ionic radius than Gd doped BiFeO3,thus Bi0.8Ho0.2Fe0.95Ti0.05O3 ceramics possessed of better magnetic properties than Bi0.8Gd0.2Fe0.95Ti0.05O3 nanoceramics.Meanwhile,a total orthorhombic structure with the introduction of Ho3+led to weakened ferroelectric properties in Bi0.8Ho0.2Fe0.95Ti0.05O3nanoceramics,and Bi0.8Ho0.2Fe0.95Ti0.05O3 nanoceramics maintained a low dielectric loss.
Keywords/Search Tags:multiferroics, BiFeO3, nanoceramcis, doping, dielectric relaxation, defect type, rhombohedral phase, orthorhombic phase
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