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Structure,Magnetic And Dielectric Properties Of B-Cr/Co-doped And A-site Zr-doped YMnO3

Posted on:2019-02-23Degree:DoctorType:Dissertation
Country:ChinaCandidate:F WanFull Text:PDF
GTID:1361330623953436Subject:Materials Physics and Chemistry
Abstract/Summary:PDF Full Text Request
Multiferroic material is a kind of multifunctional material which integrates the physical properties of ferromagnetism,ferromagnetism and ferroelastic.It has great application prospects in spintronic devices,magnetic sensors,information storage and cryogenic magnetic refrigeration systems due to the coupling effect between ferroelectricity and ferromagnetism.However,the multiferroic materials are far from the practical applications because of the deficiencies of single-phase multiferroic materials at room temperature and the weak coupling between magnetic orders and ferroelectric orders.Therefore,the exploration of multiferroic materials has been a key subject in condensed matter physics and materials science.The hexagonal YMnO3 has become one of the most popular multiferroic materials due to its novel physical properties.In this paper,we focus on hexagonal YMnO3 to discuss the influence of Cr,Co and Zr doping on the crystal structure,dielectric and magnetic properties.The main research results are as follows:?1?Cr doping at B site of a series of polycrystalline Y1-xCrxMnO3?x=0.00,0.03,0.05,0.07,0.10?compounds were synthesized in air by solid-state method.Powder X-ray diffraction gives evidence that all the samples are single phase and exhibit hexagonal structure with P63cm space group as observed for YMnO3,but the grain size decreases with increasing doping amount.The origins of dielectric relaxations of Cr doped YMnO3 were investigated by the influences of temperature and ac bias voltage on the dielectric property.The results show that the inverse S shape curve in the temperature range of 70-90 K region which is related to the magnetoelectric coupling.The obvious dielectric relaxations were observed in the temperature range of 160-280 K.This dielectric relaxation follows the Arrhenius law,which is the thermal activated process.It is found that the magnetization increases significantly with increasing doping content of Cr3+ions,and the antiferromagnetic ordered transition temperature TN increases to 86 K in the sample of x=0.10.Cr3+ions doping weakens the long-range antiferromagnetic exchange interaction between the Mn3+ions in YMnO3,and it also introduces the short-range ferromagnetic exchange intercction between Mn3+and Cr3+/Mn4+,simultaneously.The competition between the ferromagnetic exchange intercction and antiferromagnetic exchange interaction results in the decrease of magnetoresistance frustration effect of YMnO3.The hysteresis loops of Y1-xCrxMnO3 were measured at 5 K.The exchange bias field accompany horizontal magnetization shift was observsed and the exchange bias field increases with the increase of Cr3+ion doping amount.The trend of exchange bias effect with the doping concentration shows that antiferromagnet plays an important role on the pinning of ferromagnetic or uncompensated spins.Meanwhile,the YMn0.9Cr0.1O3 ceramic is processed in oxygen and nitrogen atmosphere and the effect of annealing treatment of different atmospheres on the magnetic properties of YMn0.9Cr0.1O3was studied.The results show that the increase of Mn4+ion leads to the increase of YMn0.9Cr0.1O3 ferromagnetic composition in O2 atmosphere annealing,and the significant increase of oxygen vacancy concentration is the main factor leading to the weakening of YMn0.9Cr0.1O3 ferromagnetism in the annealing of N2 atmosphere.?2?Cr doped YMnO3 single crystal with a diameter of 4-5 mm and a length of 60-80 mm was produced by high pressured floating zone technique.The primary crystal defects sub-angle grain boundaries and inclusions in the crystal have been investigated by X ray diffraction and scanning electron microscopy.The formation mechanisms of these defects were discussed and the relevant approaches of restraining these defects have also been presented,which essential to optimize the growth parameters and improve crystal quality.?3?B site substitution of Y1-xCoxMnO3?x=0.00,0.03,0.05,0.07,0.10?samples are prepared by standard solid state sintering method.The X-ray diffraction and Raman scattering spectra show that the samples are of hexagonal phase with group P63cm when x?0.07.While x>0.07,the hexagonal phase with group P63cm and the orthorhombic phase with group Pbnm coexist in those samples.It is shown that the ferroic magnetization and the peak of-?SM-T curve increase with the increasing of Co doping and the maximum magnetic entropy change and the ferroic magnetization follow a non-linear relationship.The introduction of ferromagnetic exchange between Mn2+and Mn3+in addition to the ferromagnetic exchange between Mn3+and Mn4+cuases the increasing magnetization.The dielectric test results show that there is an intrinsic dielectric relaxation of the thermal activation process at the temperature range of350-650 K.?4?Zr doping at A-site of Y1-xZrxMnO3?x=0.00,0.05,0.10?polycrystalline samples were prepared by solid-state method under air atmosphere.The Curie temperature,Curie constant and the effective magnetic moment were systematically analyzed.The results suggest that the ferromagnetic composition increases with the increase of doping amount and the samples enter the spin glass state below 15 K.This is related to the competition between ferromagnetic double exchange and antiferromagnetic super-exchange,and the antiferromagnetic tilt is also an important factor.
Keywords/Search Tags:Multiferroic materials, YMnO3, Solid state sintering method, Floating zone method, Doping, Magnetic property, Dielectric property
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