BNKT BZN无铅压电陶瓷的制备及电学性能研究

采用传统固相法制备得到(0.8-x) Bi0.5 Na0.5TiO3-0.2Bi0.K0.5TiO3-xBi(Zn2/3 Nb1/3)O3(摩尔分数0≤x≤0.06)(简称(0.8-x)BNT-0.2BKT-xBZN)无铅压电陶瓷.利用XRD、SEM等测试技术表征了该体系陶瓷的晶体结构、表面形貌及介电和压电性能.研究结果表明,所有组分的陶瓷样品均形成典型的钙钛矿结构;同一烧结温度下,随着Bi(Zn2/3 Nb1/3)O3含量的增加,晶粒尺寸增加;在1 180℃烧结温度保温2h的条件下,组成为x=0.02的陶瓷样品经极化后,压电常数d33=48 pC/N,相对介电常数ε33T/ε0=598.9,介电损耗tan δ=0.048 45.     

(La0.44Sr0.33)TiO3对MgTiO3系高频高Q MLCC瓷料性能的影响

采用传统固相反应法制备了(1-x)(Mg0.95Zn0.05)TiO3-x(La0.44Sr0.33)TiO3(MZLST)介质陶瓷。系统研究了(La0.44Sr0.33)TiO3掺杂量对MZLST陶瓷烧结特性、相构成、微观结构和微波介电性能的影响。结果表明,掺杂少量的(La0.44Sr0.33)TiO3后,MZLST陶瓷的主晶相为(Mg0.95Zn0.05)TiO3和(La0.44Sr0.33)TiO3,随着烧结温度的升高,第二相(Mg0.95Zn0.05)Ti2O5的含量增加。当x=0.10时,MZLST陶瓷在1 285℃烧结2h获得最佳的介电常数εr=22.17,品质因数Q.f=48 471GHz(6.72GHz),谐振频率温度系数τf=-7.99×10-6/℃。     

添加TiO2的ZnNb2O6陶瓷的相结构和性能

采用传统的固相合成法制备ZnNb2O6与TiO2摩尔比为1∶x系统微波陶瓷,借助XRD、SEM和LCR测试仪,研究了TiO2添加对ZnNb2O6陶瓷的烧结特性、相组成结构及介电性能.结果表明,随着TiO2含量的增加,晶相结构变得复杂化,TiO2掺杂质量分数x＜0.4时,只有ZnNb2O6晶相;0.6＜x＜1.4时,存在ZnNb2TiO8、Zn0.17Nb0.33Ti0.5O2和Zn0.15Nb0.3Ti0.55O2三相;1.6＜x＜2.0时,由ZnNb2TiO8和TiO2两相组成.同时,随着相结构的变化,陶瓷的介电常数εr增加,品质因数Q值先减小后增大,频率温度系数τf向正方向移动.在1 200℃烧结(x=1.8)的陶瓷具有较佳的微波性能:εr=51,Q×f=11 187 GHz,τf=-8μ℃-1.     

(Zn_(0.9)Mg_(0.1))TiO_3微波介质陶瓷低温烧结研究

采用传统固相法对使用Mg取代一部分Zn形成的六方钛铁矿型无限固溶体(Zn0.9Mg0.1)TiO3陶瓷进行了低温烧结研究。低熔点玻璃ZnO-B2O3-SiO2(ZBS)的加入提高了烧结致密度,使烧结温度降低到900℃以下,制得了不含Zn2TiO4的单一六方(Zn0.9Mg0.1)TiO3相陶瓷,其微波介电性能优异。加入质量分数为0.5%的ZBS玻璃时,在900℃成瓷良好,介电常数εr=20.53,品质因数与频率的乘积Q×f=61 630GHz(f=7.4GHz)。     

Zn0.9Mg0.1Al2O4微波导热陶瓷材料的改性研究

采用固相反应法烧结制备了具有较高热导率的Zn0.9Mg0.1Al2O4 +x%TiO2 (质量分数0≤x≤3)微波介质陶瓷,并研究了TiO2对Zn0.9Mg0.1Al2O4陶瓷的晶相、微观形貌、微波介电和导热性能的影响。研究表明,随着TiO2掺杂量增加,Zn0.9Mg0.1Al2O4陶瓷中会出现少量非化学计量数化合物产生的相。同时,掺杂TiO2会促进晶粒生长。这是由于掺杂TiO2促进了烧结反应的进行,同时也抑制了微观晶格紊乱和宏观偏析,使Zn0.9Mg0.1Al2O4陶瓷的介电与导热性能得到提升。结果表明,Zn0.9Mg0.1Al2O4+2%TiO2陶瓷在1 500 ℃烧结时具有最佳的介电与导热性能,介电常数εr =8.57,品质因数与频率之积Q×f = 180 861 GHz,热导率为19.67 W/(m ·K)。     

烧成工艺对(MgZn)TiO3微波介质陶瓷性能的影响

以(MgCO3)4·Mg(OH)2·5H2O、ZnO、TiO2为原料,固相反应法烧结成瓷.运用XRD、SEM、阻抗分析仪和网络分析仪对(Mgt1-(x)Zn(x))TiO3(MZT)材料的相组成、微观显微结构及微波介电性能进行分析.系统研究了预烧温度对MZT系统介电性能的影响.结果表明,不同的预烧工艺可影响MZT材料的烧结性能和微波介电性能.(Mg0.9Zn0.1)TiO3材料1 170℃预烧,1 250℃烧结时,具有较好的介电性能:介电常数εr=17.7,品质因数Q·(f)=0.1 PHz.频率温度系数(τ(f))约为-79X10-6/℃.(Mg0.7Zn0.3)TiO3材料1 100℃预烧,1 250℃烧结时,其εr=18.7,Q·(f)=90 THz,τ(f)约为-50×10-6/℃.     

ZnO掺杂MgTiO3-CaTiO3陶瓷的介电性能

采用固相反应法制备 (Mg0.95-xZnxCa0.05)TiO3介质陶瓷.研究了ZnO掺杂对MCT陶瓷介电性能的影响.结果表明,ZnO掺杂的MCT陶瓷的主晶相为MgTiO3和CaTiO3两相结构,随着ZnO掺杂量的增加,有第二相产生,为Zn2TiO4.ZnO掺杂能降低MCT陶瓷的烧结温度到1 250 ℃,且对介电常数温度系数αc 有调节作用.当 x=0.02时在1 250 ℃温度烧结2.5 h获得最佳性能,即介电常数εr =21.7,介电损耗 tan δ=1×10-5,介电常数温度系数αc =2.12×10-5.     

(Mg_(0.7)Zn_(0.3))TiO_3-(Ca_(0.61)La_(0.26))TiO_3系微波介质陶瓷性能研究

采用传统固相反应法制备了(1-x)(Mg0.7Zn0.3)TiO3-x(Ca0.61La0.26)TiO3(MZCLT)微波介质陶瓷。分析了(Ca0.61La0.26)TiO3掺杂量对MZCLT陶瓷相结构、烧结性能和介电性能的影响。所制MZCLT陶瓷的主晶相为(Mg0.7Zn0.3)TiO3和(Ca0.61La0.26)TiO3,还存在微量的(Mg0.7Zn0.3)Ti2O5。当x=0.13,1275℃烧结4h时,0.87(Mg0.7Zn0.3)TiO3-0.13(Ca0.61La0.26)TiO3陶瓷介电性能较佳:εr=26.7,Q·f=86011GHz(8GHz),τf为-6×10-6/℃,优于(Mg0.7Zn0.3)TiO3陶瓷介电性能(εr=19.2,Q·f=253000GHz,τf为-39×10-6/℃)。     

ZrO2掺杂对Ba(Zn1/3Ta2/3)O3陶瓷介电性能的影响

采用固相反应烧结法制备了ZrO2掺杂的Ba(Zn1/3Ta2/3)O3微波介质陶瓷,研究了陶瓷的烧结特性和介电性能。结果表明,ZrO2掺杂能有效降低Ba(Zn1/3Ta2/3)O3陶瓷的烧结温度,改善陶瓷的微波介电性能。当x(ZrO2)=4%时,Ba(Zn1/3Ta2/3)O3陶瓷致密化烧结温度由纯相时的1 600℃降至1 300℃,同时陶瓷材料的微波介电性能达到最佳值,即介电常数εr=34.79,品质因数与频率的乘积Q×f=148 000(8GHz),谐振频率温度系数τf=0.3×10-6/℃。     

Sb2O3掺杂Zn-Nb-O基微波介质陶瓷的结构与性能

采用传统电子陶瓷工艺制备(ZnNb2O6-Zn3Nb2O8)-Sb2O3(ZZS)陶瓷,研究了Sb2O3含量对ZZS陶瓷结构及介电性能的影响规律。结果表明,Sb2O3的加入促进了陶瓷的烧结,陶瓷中除ZnNb2O6和Zn3Nb2O8两种主晶相外未有新相生成,Sb2O3则以Sb3+或Sb5+置换Nb5+/Zn2+形成置换固溶体;陶瓷的介电常数(εr)随Sb2O3含量的增加先增大后减小,保持在23～25之间,介电损耗略有增加。微波频段下,0.7ZnNb2O6-0.3Zn3Nb2O8陶瓷的介电常数随Sb2O3含量的增加略有减小,品质因数与频率的乘积(Q×f)值先增大后减小。当w(Sb2O3)=1%时,陶瓷综合性能最佳,εr=22.88,Q×f=38 871GHz。     

Theoretical investigation of mechanical,optoelectronic and thermoelectric properties of BiGaO3 and BiInO3 compounds

The cubic BiGaO₃ and BiInO₃ perovskite oxides have been investigated for their structural stability, mechanical and opto-electronic properties by employing the density functional theory. The exchange-correlation effects have been modeled with Perdew–Burke–Ernzerhof generalized gradient approximation, while the improved evaluation of electronic properties has been achieved by using the Tran–Blaha modified form of semi-local Becke–Johnson functional. Structural properties are calculated and the thermodynamics stability of BiGaO₃ and BiInO₃ in the cubic perovskite structure has been established in terms of enthalpies of formation. Furthermore, elastic coefficients such as C_ij, bulk modules B, anisotropy factor, shear modulus G, Young’s modulus Y, Poisson’s ratio ν, and B/G ratio are predicted. Band structure calculations reveal that investigated compounds have an indirect band gap between the occupied O 2p and unoccupied Bi 6p orbitals. The optical response of BiGaO₃ and BiInO₃ are also inspected by computing the complex dielectric function, refractive index, absorption coefficient, extinction coefficient, reflectivity and optical conductivity for radiation with energy up to 16 eV. The important thermoelectric properties of the compounds are described in terms of thermal conductivity, electrical conductivity, Seebeck coefficient and figure of merit.     

铅镁锰锑铌多元系压电陶瓷材料

采用先驱体法制备了Pb(Mg_(1/3)Nb_(2/3))_A(Mn_(1/3)Nb_2/3))_B(Mm_(1/3)Sb_(2/3))_CZr_DTi_EO_3(PMMSN)铅镁锰锑铌多元系中温压电陶瓷材料。从XRD图谱可以看出,先驱体法容易消除焦绿石相,得到单相钙钛矿材料。实验结果表明,先驱体法制成样品的烧成温度较低,压电和介电性能优良。1100℃烧结样品的性能参数:Qm为2060,k_p为0.55,ε_r为1200,d_(33)为293 pC/N,tgδ为0.45×10~(-2),可用于压电变压器、超声换能器和压电马达等功率型器件。     

碳酸钙对BaTiO_3系PTC热敏电阻电性能的影响

研究了碳酸钙对ＢａＴｉＯ３ 系ＰＴＣ热敏电阻电性能的影响。结果表明,随着钙加入量的增加,ＢａＴｉＯ３ 的低温相变点, 移向更低的温度; 促进烧成时芯片的致密化; 使ＢａＴｉＯ３ 晶粒尺寸几乎呈线性下降; 使晶粒、晶界电阻下降; α、Ｒｍ ａｘ／Ｒｍ ｉｎ 无大的变化, ρ２５增大, Ｖｂ 提高。碳酸钙的理化指标, 对ＰＴＣ热敏电阻电性能也有很大影响, 据此推荐了ＢａＴｉＯ３ 系ＰＴＣ热敏电阻用ＣａＣＯ３ 的技术标准     

Ba(Zn1/3Nb2/3)O3-BaZrO3系统结构和介电性能的研究

研究了BaZrO3、MnCO3对Ba(Zn1/3Nb2/3)O3(BZN)系统结构和介电性能的影响。表明BaZrO3及Mn-CO3均能有效降低系统的烧结温度。系统中加入过多的BaZrO3(BZ)会降低介电常数,增大介质损耗,并使容量温度系数负向发展;加入微量MnCO3对系统的介电性能影响不大。系统中加入的x(BaZrO3)=4%会生成较多的第二相BaNb2O6、BaZrO3摩尔分数增加至8%时,第二相消失。这是由于过多BZ的加入会在烧结温度到达前生成较多液相,促进烧结的同时也阻碍了ZnO的挥发,从而抑制了第二相的生成。向96%BZN-4%BZ中加入r(MnCO3)=0.5%,也会抑制第二相的生成,这可能是由于Mn2+占据了B′位Zn2+挥发后留下的空位,形成固溶体,没有形成富Nb液相区,从而抑制了第二相的生成。     

Structural and magnetic properties of Dy3+ doped Y3Fe5O12 for microwave devices

The Dy³⁺ doped Y_3−xDy_xFe₅O₁₂ (x=0–3) nanopowders were prepared using microwave hydrothermal route. The structural and morphological studies were analyzed using transmission electron microscope, X-ray diffractometer and field emission scanning electron microscope. The nanopowders were sintered at 900 °C/90 min using microwave furnace. Dense ceramics with theoretical density of around 95% was obtained. Ferro magnetic resonance (FMR) spectrum and microwave absorption spectrum of Dy³⁺ doped YIG were studied, the signal exhibits a resonance character for all Dy³⁺ variations. It was observed that the location of the FMR signal peak at the field axes monotonically shifts to higher field with increasing Dy³⁺ content. The dielectric and magnetic properties (ε′, ε′′, µ′ and µ′′) of Dy³⁺ doped YIG were studied over a wide range of frequency (1–50 GHz). With increase of Dy³⁺ both ε′ and µ′ decreased. The low values of dielectric, magnetic properties and broad distribution of FMR line width of these ceramics are opening the real opportunity to use them for microwave devices above K- band frequency.     

先驱体法制备Pb1-xSrx(Mn1/3Sb2/3)aZrbTicO3压电陶瓷的压电和介电性能

采用先驱体法制备了Pb1-xSrx(Mn1/3Sb2/3)aZrbTicO3压电陶瓷。通过XRD研究表明,随着Sr2+取代量的增加,相界向富锆方向移动,并改善了相界附近组分的压电性能和介电性能。与传统的固相合成制备工艺相比,先驱体法制备的陶瓷具有优良的压电性能,所得样品的综合性能:r为1791,tg为0.0035,d33为454?0-12C種-1,kp为0.61。     

Characterization of Bi2S3 nanorods prepared at room temperature

Bi₂S₃ is a direct band gap semiconductor with a band gap of 1.3 eV. It belongs to the family of metal chalcogenides of type A₂^VB₃^VI (A=As, Sb, and Bi; B=S, Se, and Te), whose importance in photovoltaic and thermoelectric applications is well recognized. Although nanostructures of Bi₂S₃ have been obtained using a number of techniques, reports on assemblies of Bi₂S₃ are sparse. In the present work, we prepared single crystalline bismuth sulfide (Bi₂S₃) nanorods at room temperature by reacting Bi(NO₃)₃, thioacetamide (TAA), hydrochloric acid and distilled water.Energy dispersive analysis of X-rays (EDAX) obtained from Bi₂S₃ nanorods indicated no incorporation of other foreign impurities in it. X-ray diffraction confirmed the single phase of Bi₂S₃ and different diffracting planes were indexed based on the orthorhombic structure and lattice parameters were determined. X-ray photoelectron spectroscopy (XPS) was used to evaluate its composition and purity. The synthesized nanorods with different images observed under transmission electron microscopy (TEM) are shown in the paper and the selected area electron diffraction (SAED) pattern obtained from these nanorods shows their single crystalline behavior. Raman measurement performed at room temperature using Ar⁺ laser (488 nm) confirms the presence of 238 cm⁻¹ and 972 cm⁻¹ phonon modes. The optical absorption spectra obtained by UV–vis spectrometer show blue shift in comparison to bulk Bi₂S₃ while its thermal stability was studied by thermogravimetric analysis.     

MnCO3掺杂对BaTiO3-Nb2O5-CO3O4陶瓷性能的影响

为了提高BaTiO3-Nb2O5-Co3O4( BNC)陶瓷的介电常数,采用传统固相反应法制备了MnCO3掺杂的BNC陶瓷,研究了MnCO3掺杂量以及烧结温度对BNC陶瓷致密度及介电性能的影响.结果表明:MnCO3的掺杂提高了BNC陶瓷的介电常数,降低了介质损耗.当MnCO3掺杂量为摩尔分数0.5％时,BNC陶瓷相对介...     

Elastic and optoelectronic properties of novel Ag3AuSe2 and Ag3AuTe2 semiconductors

Ag₃AuSe₂ and Ag₃AuTe₂ are interesting class of semiconducting materials. Here, elastic and opto-electronic properties of Ag₃AuSe₂ and Ag₃AuTe₂ semiconductors are studied in detail using density functional theory. Different schemes are selected to treat the exchange-correlation effects. The unit cell of the compounds is fully optimized and calculated cell constants are found in agreement to the existing experimental data. The calculated elastic constants and elastic moduli reveal that the compounds possess ductile nature and are elastically stable. It is found that both compounds are direct bandgap semiconductor with bandgap value of 1.009 eV for Ag₃AuSe₂ and 0.551 eV for Ag₃AuTe₂. As the compounds have narrow and direct bandgaps, therefore optically active. The optical properties like reflectivity, absorption coefficient, energy loss function, refractive index including and complex dielectric function are studied in detail. The direct band gap nature of these compounds make them useful candidate for different devices applications.