物理学报
物理學報
물이학보
2013年
7期
356-363
,共8页
张德明%庄重%王先平%方前锋
張德明%莊重%王先平%方前鋒
장덕명%장중%왕선평%방전봉
氧离子导体%La1.9Y0.1Mo2O9%细晶粒陶瓷%微波烧结
氧離子導體%La1.9Y0.1Mo2O9%細晶粒陶瓷%微波燒結
양리자도체%La1.9Y0.1Mo2O9%세정립도자%미파소결
oxide-ion conductors%La1.9Y0.1Mo2O9%fine-grain ceramic%microwave sintering method
采用溶胶凝胶法合成的La1.9Y0.1Mo2O9纳米晶粉体,结合微波烧结技术制备出不同晶粒度的La1.9Y0.1Mo2O9块体样品.利用X射线衍射仪(XRD)、高分辨透射显微镜(HRTEM)、场扫描显微镜(SEM)对粉体及陶瓷块体的物相、形貌进行了表征,利用交流阻抗谱仪测试了样品不同温度下的电导率.实验结果表明,掺Y的La1.9Y0.1Mo2O9能将高温立方β相稳定到室温;块体样品致密均匀,平均晶粒度范围在60 nm—4μm之间;致密度高的样品表现出高的电导率,其中900?C烧结样品的电导率600?C时高达0.026 S/cm,比固相反应法制备的La1.9Y0.1Mo2O9样品高出约1倍.总结认为样品的致密性对电导率影响较大,是通过影响晶界电导率来影响总电导率的,样品的晶粒度(在60 nm—4μm范围内)对电导率的影响还不能确定.
採用溶膠凝膠法閤成的La1.9Y0.1Mo2O9納米晶粉體,結閤微波燒結技術製備齣不同晶粒度的La1.9Y0.1Mo2O9塊體樣品.利用X射線衍射儀(XRD)、高分辨透射顯微鏡(HRTEM)、場掃描顯微鏡(SEM)對粉體及陶瓷塊體的物相、形貌進行瞭錶徵,利用交流阻抗譜儀測試瞭樣品不同溫度下的電導率.實驗結果錶明,摻Y的La1.9Y0.1Mo2O9能將高溫立方β相穩定到室溫;塊體樣品緻密均勻,平均晶粒度範圍在60 nm—4μm之間;緻密度高的樣品錶現齣高的電導率,其中900?C燒結樣品的電導率600?C時高達0.026 S/cm,比固相反應法製備的La1.9Y0.1Mo2O9樣品高齣約1倍.總結認為樣品的緻密性對電導率影響較大,是通過影響晶界電導率來影響總電導率的,樣品的晶粒度(在60 nm—4μm範圍內)對電導率的影響還不能確定.
채용용효응효법합성적La1.9Y0.1Mo2O9납미정분체,결합미파소결기술제비출불동정립도적La1.9Y0.1Mo2O9괴체양품.이용X사선연사의(XRD)、고분변투사현미경(HRTEM)、장소묘현미경(SEM)대분체급도자괴체적물상、형모진행료표정,이용교류조항보의측시료양품불동온도하적전도솔.실험결과표명,참Y적La1.9Y0.1Mo2O9능장고온립방β상은정도실온;괴체양품치밀균균,평균정립도범위재60 nm—4μm지간;치밀도고적양품표현출고적전도솔,기중900?C소결양품적전도솔600?C시고체0.026 S/cm,비고상반응법제비적La1.9Y0.1Mo2O9양품고출약1배.총결인위양품적치밀성대전도솔영향교대,시통과영향정계전도솔래영향총전도솔적,양품적정립도(재60 nm—4μm범위내)대전도솔적영향환불능학정.
A series of La1.9Y0.1Mo2O9 bulk samples of different grain sizes were made by microwave sintering the nanocrystalline powders prepared by sol-gel methods. Phases, microstructure, grain size of the powders and bulk samples were examined by using X-ray diffraction (XRD), high-resolution transmission electron microscope (HRTEM) and scanning electron microscope (SEM); and the electrical properties of the bulk samples were studied by AC impedance spectroscopy. Experimental results show that the substituent Y can stabilize the cubicβ phase to room temperature;the bulk samples are dense and uniform with an average grain size from 60 nm to 4 μm;the highly dense bulk samples show enhanced ionic conduction, e.g. the conductivity of the sample with relative density 99%is 0.026 S/cm at 600 ?C, which is two times higher than that of bulk samples prepared by solid-state reaction. It can be concluded that the effect of sample density on the electrical conductivity is mainly due to the grain boundary conductivity;and the effect of sample grain size (from 60 nm to 4 μm) on the electrical properties is not so significant.