ZnO-MgO-TiO_2-SnO_2系高频介电陶瓷的制备与介电性能

在ZnO-TiO2-SnO2陶瓷基础上,掺杂MgO得到(1-x)ZnO-xMgO-0.88TiO2-0.12SnO2系新型介电陶瓷。对其相转变、微观组织结构和高频介电性能进行了研究,结果表明,在不加入任何烧结助剂情况下,试样可于1 080℃达到烧结,其相对密度为94.4%;当x=0.05时,陶瓷为纯相尖晶石结构(Zn0.95,Mg0.05)2(Ti0.88,Sn0.12)O4,其介电性能优良,1 MHz时ε=18.88,tanδ=5×10-4,τε=2.89×10-6/℃,可用作高频电容器材料的优秀候选材料。     

Zn-Al共掺对0.95MgTiO3-0.05CaTiO3介电性能的影响

采用固相反应法制备了(Mg0.93Ca0.05Zn0.02)(Ti1-xAlx)O3介质陶瓷.研究了Zn-Al共掺杂对0.95MgTiO3-0.05CaTiO3(95MCT)陶瓷介电性能的影响.结果表明:Zn-Al共掺杂的95MCT陶瓷的主晶相为MgTiO3和CaTiO3两相结构,Zn-Al共掺杂可以抑制中间相MgTi2O5的产生,同时,有第二相CaAl2O4出现;Zn-Al共掺杂能有效地降低95MCT陶瓷的烧结温度至1300℃,改善介电性能,并对介电常数温度系数具有调节作用.当 Zn2+掺杂量为0.02mol、Al3+掺杂量为0.02mol时, 在1300℃烧结2.5h获得最佳性能:εr =20.35, tgδ=2.0×10-6, αc=-1.78×10-6.     

(Ba1-xSrx)La4Ti4O15（x=0.8～0.95）陶瓷的微结构及微波介电性能研究

采用固相反应法制备了(Ba1-xSrx)La4Ti4O15(x=0.8~0.95)复合体系微波介质陶瓷,并对其进行物相组成、晶体结构分析以及微波介电性能的研究.研究结果表明,(Ba1-xSrx)La4Ti4O15陶瓷主晶相为SrLa4Ti4O15,并伴随有第二相SrLa8Ti9O15.SEM观察表明,Ba0.2Sr0.8La4Ti4O15陶瓷内部微观结构致密,晶粒尺寸在10~20μm之间,晶界清晰.随着x值逐渐增大,(Ba1-xSrx)La4Ti4O15陶瓷中晶粒形态发生变化,气孔增多.在x=0.8时,(Ba1-xSrx)La4Ti4O15陶瓷具有优良的微波介电性能,即εr=40.86,Q×f≈62806 GHz,τf=20×10 6/℃.随着Ba2+的含量逐渐增加,该陶瓷的介电常数εr单调上升,品质因子Q×f值增加,说明适量的Ba2+替代Sr2+能改善陶瓷的微波介电性能.     

复合添加La_2O_3/MgO对(Zr_(0.8)Sn_(0.2))TiO_4陶瓷性能的影响

讨论了复合添加La2O3/MgO对(Zr0.8Sn0.2)TiO4介质陶瓷烧结机制和微波介电性能的影响。结果表明,La2O3/MgO对(Zr0.8Sn0.2)TiO4的烧结有一定的促进作用,但La2O3/MgO添加量的增大会造成晶格缺陷和残留气孔的增多,从而导致材料的密度和Q×f降低。在1320℃保温12h、La2O3/MgO添加量为0.9wt%时,(Zr0.8Sn0.2)TiO4介电性能最好,其εr=37.14,Q×f=36600,τf=7.77×10-6/℃。     

CaTiO3 对(1-x)ZnAl2O4-xMg2TiO4(x=0.21)微波介质陶瓷结构和性能的影响

利用常规固相法制备了ZnAl2O4-Mg2TiO4-CaTiO3陶瓷,研究了CaTiO3对其相成分、微观组织结构和微波介电性能的影响规律. 结果表明,CaTiO3能有效地改善(1-x)ZnAl2O4-xMg2TiO4(x=0.21)材料的烧结性能,使其致密化温度降低150℃. ZnAl2O4-Mg2TiO4-CaTiO3陶瓷体系中包括ZnAl2O4基尖晶石相、CaTiO3、MgTi2O5和Zn2Ti3O8相,当烧结温度高于1400℃时,Zn2Ti3O8相消失. 随着CaTiO3含量的增加,体系中CaTiO3相含量增加而MgTi2O5相含量减少,且CaTiO3具有显著地调节谐振频率温度系数的作用. 当在(1-x)ZnAl2O4-xMg2TiO4(x=0.21)体系中掺入6mol%的CaTiO3添加剂时,经1400℃烧结后能获得温度稳定性好的微波介质陶瓷材料,其微波介电性能为:εr=11.8,Q*f=88080GHz,τf=-7.8×10-6/℃.     

(1-x)(Mg0.7Zn0.3)TiO3-xCa0.61La0.26TiO3系陶瓷的微波介电性能研究（英文）

本实验研究了(1-x)(Mg0.7Zn0.3)TiO3-x(Ca0.61La0.26)TiO3(MZT-CLT)系陶瓷的微观结构和微波介电性能,通过(Ca0.61La0.26)TiO3来协调(Mg0.7Zn0.3)TiO3陶瓷的谐振频率温度系数.MZT-CLT陶瓷的主晶相为(Mg0.7Zn0.3)TiO3,第二相为Ca0.61La0.26TiO3和(Mg0.7Zn0.3)Ti2O5.烧结温度和陶瓷组成对微波介电性能影响显著,当烧结温度为1275℃时,可以获得良好的致密度,当烧结温度超过1300℃时,Zn的蒸发导致陶瓷致密度和介电性能下降.随着(Ca0.61La0.26)TiO3含量的增大,材料的介电常数增大,品质因数减小.当x=0.13,烧结温度为1275℃保温4h,(MZT-CLT)陶瓷具有优良微波介电性能,εr=26,Q.f=86000 GHz,τf=-6×10-6/℃.     

(Mg1-xSrx)2Al4Si5O18陶瓷的显微结构与微波介电性能研究

采用固相烧结反应法制备(Mg1-xSrx)2Al4Si5O18陶瓷.Sr掺杂促进低温相β-Mg2Al4Si5O18向高温相α-Mg2Al4Si5O18转变,并拓宽了(Mg1-xSrx)2Al4Si5O18陶瓷的致密化烧结温度范围.X射线衍射结果表明在0≤x<0.2范围内,(Mg1-xSrx)2Al4Si5O18陶瓷以(Mg,Sr)2Al4Si5O18堇青石固溶体形式存在;在0.6相似文献   

Bi4Ti3O12掺杂对(Bi1.5Zn0.5)(Zn0.5Nb1.5)O7陶瓷结构与介电性能的影响

研究了Bi4Ti3O12掺杂对(Bi1.5Zn0.5)(Zn0.5Nb1.5)O7(BZN)陶瓷烧结特性、相结构和介电性能的影响.采用传统的固相反应法制备样品,X射线衍射技术分析相结构,SEM观察表面形貌.结果表明,Bi4Ti3O12掺杂能有效地促进烧结,提高介电常数ε,降低介电损耗tgδ,优化介电频率温度系数αε.1000℃烧结8%(摩尔分数) Bi4Ti3O12掺杂的BZN陶瓷具有较好的介电性能ε=192,tgδ= 4.21×10-4,αε=-3.37×10-4/℃.     

(Mg_(1-x)Zn_x)_2SiO_4(0≤x≤1)陶瓷微波介电性能研究

采用固相反应法制备(Mg1-xZnx)2SiO4(0≤x≤1)微波介质陶瓷,研究(Mg1-xZnx)2SiO4陶瓷在0≤x≤1范围内的相演变、微结构与其微波介电性能间相互关系.XRD测试结果表明:橄榄石结构的Mg2SiO4与硅矽矿结构的Zn2SiO4在晶体结构上存在很大差别,(Mg,Zn)2SiO4在0≤x≤1范围内只能部分地实现有限固溶.背散射电子扫描显微镜(BESEM)测试结果显示:随着x的增加,MgSiO3第二相得到抑制;陶瓷出现液相烧结,促进晶粒生长与玻璃相在晶界处沉积.微波介电性能测试结果表明:由于Zn2+离子极化能力大于Mg2+离子,(Mg1-xZnx)2SiO4(0≤x≤1)陶瓷介电常数随x值增加而增大;0≤x≤1范围内,Mg2SiO4陶瓷微波性能由于第二相、气孔率增加与晶粒增大而降低,Zn2SiO4陶瓷由于微结构得到改善,陶瓷微波性能得到优化.当x=0.6时,得到较好的(Mg0.4Zn0.6)2SiO4陶瓷微波性能为:εr=6.6,Qf=95650GHz,τf=-60×10-6/℃.     

Ca[(Li_(1/3)Nb_(2/3))_(0.8)Sn_(0.2)]O_(3-δ)-xTiO_2陶瓷的微波介电特性

研究了Ca[(Li1/3Nb2/3)0.8Sn0.2]O3-δ-xTiO2(0≤2≤0.2)陶瓷的微观结构及微波介电特性.当0≤x≤10%(摩尔分数,下同)时,体系为单一钙钛矿相.随Ti4+含量的增加,B位1:2有序度下降,品质因素减小,谐振频率温度系数先由-22.6×10-6/℃增加到-11.1×10-6/℃,然后向负值方向移动.当Ti4+含量为10%时,陶瓷微波介电性能最佳:εr=29.3,Qf=2684GHz,τf=-11.1×10-6/℃.     

La0.5Y0.5Ni4.8Mn0.1Al0.1和La0.5Y0.5Ni4.8Al0.2合金的储氢性能研究

针对两种新型稀土型储氢合金La0.5Y0.5Ni4.8Mn0.1Al0.1和La0.5Y0.5Ni4.8Al0.2的储氢特性进行研究分析。实验表明,相同温度下,La0.5Y0.5Ni4.8Mn0.1Al0.1和La0.5Y0.5Ni4.8Al0.2合金的PCT曲线基本重合,且都具有优良的吸氢动力学性能;相比之下,后者的滞后系数要小于前者,吸氢量较大,吸氢速率也较快,故其储氢性能较优。300次吸放氢循环实验结果表明,La0.5Y0.5Ni4.8Al0.2合金的吸氢动力学性能虽然略有下降,但抗粉化性能较好。     

Dy0.6Tb0.3Pr0.1(Fe0.95Mn0.05)x取向晶体的结构与磁致伸缩

采用Ｃｚｏｃｈｒａｌｓｋｉ方法生长了Ｄｙ０．６Ｔｂ０．３Ｐｒ０．１（Ｆｅ０．９５Ｍｎ０．０５）ｘ（１．８５≤ｘ≤１．９５）取向合金。所有合金主相为立方Ｌａｖｅｓ相结构,择优取向不完整择优取向的方向与Ｘ的大小有关。研究了沿着这些样品的生长方向的磁致伸缩性能以及磁致伸缩性能与压力之间的关系。     

Thermal Stability of Amorphous Hydride Mg_(50)Ni_(50)H_(54) and Mg_(30)Ni_(70)H_(45)

The thermal stability of amorphous ternary hydrides Mg_(50)Ni_(50)H_(54) and Mg_(30)Ni_(70)H_(45) and their corre-sponding amorphous binary alloys Mg_(50)Ni_(50) and Mg_(30)Ni_(70) were studied with X-ray diffraction(XRD) and differential scanning calorimetry(DSC). Samples of the amorphous alloys were preparedby mechanical alloying and the amorphous hydrides were obtained by charging the alloys with gas-eous hydrogen at 3.0 MPa and 423 K. It was found that the amorphous hydrides released most oftheir hydrogen before the crystallization of the essentially hydrogen depleted amorphous alloy. Thecrystallization temperature of amorphous Mg_(50)Ni_(50)H_(54) elevated and that of amorphousMg_(30)Ni_(70)H_(45) did not change in relation to the original binary amorphous alloy. This is very excep-tional for amorphous hydrides. The reason for the effects of hydrogen absorption/desorption on thecrystallization of amorphous alloys was discussed.     

Zr65Al7.5Ni10Cu15Co2.5合金的玻璃转变温度

根据Ｚｒ６５Ａｌ７。５Ｎｉ１０Ｃｕ１５Ｃｏ２。５合金的纳米晶，晶体，液体和玻璃比热的测量结果，研究了合金的玻璃转变温度与全金的热力学函数，动力学参数以及加热速度的关系。结果表明，非晶态合金玻璃转变所需转变激活能很小，玻璃转变温度实际上是由于加热速度引起的不同状态的玻璃与液体的热力学平衡温度。     

Acousto-optic interaction in alpha-BaB(2)O(4)and Li(2)B(4)O(7) crystals

Experimental studies and analysis of acousto-optic diffraction in alpha-BaB(2)O(4) and Li(2)B(4)O(7) crystals are given. Ultrasonic wave velocity, elastic compliance and stiffness coefficients, and piezo-optic and photoelastic coefficients of alpha-BaB(2)O(4) and Li(2)B(4)O(7) crystals are determined. The acousto-optic figure of merit has been estimated for different possible geometries of acousto-optic interaction. It is shown that the acousto-optic figures of merit for alpha-BaB(2)O(4) crystals reach the value M(2)=(270 +/- 70) x 10(-15) s(3)/kg for the case of interaction with the slowest ultrasonic wave. The directions of propagation and polarization of those acoustic waves are obtained on the basis of construction of acoustic slowness surfaces. The acousto-optic diffraction is experimentally studied for alpha-BaB(2)O(4) and Li(2)B(4)O(7) crystals.     

Nanomechanical characterization of one-step combustion-synthesized Al(4)B(2)O(9) and Al(18)B(4)O(33) nanowires

Two kinds of aluminum borate nanowires, Al(4)B(2)O(9) and Al(18)B(4)O(33), were successfully synthesized by a one-step combustion method through control of the Al:B atomic ratio and synthesis temperature. Both nanowires are single crystalline but have distinguishing growth habits. Nanoindentation tests were performed directly on individual nanowires to reveal their mechanical properties. A 70% reduction in elastic modulus was found in Al(18)B(4)O(33) nanowires compared with their bulk counterpart. Al(18)B(4)O(33) nanowires exhibited higher hardness and elastic modulus than Al(4)B(2)O(9) nanowires.     

Plasma surface treatments of poly(l-lactic acid) (PLLA) and poly(hydroxybutyrate-co-hydroxyvalerate) (PHBV)

The surfaces of poly(l-lactic acid) (PLLA) and poly(hydroxybutyrate-co-hydroxyvalerate) (PHBV) were modified by oxygen and nitrogen plasma treatments. The physical and chemical surface characteristics were evaluated by contact angle tests, scanning electron microscopy (SEM), atomic force microscopy (AFM), and X-ray photoelectron spectroscopy (XPS). The plasma treatments caused an increase in both contact angle and roughening, altered the surface morphology, inserted polar groups, and, consequently, enhanced the hydrophilicity for both PLLA and PHBV polymers.     

Natural Passivity of Amorphous Fe_(40)Ni_(40)P_(14)B_6 and Fe_(54.6)Ni_(38)Si_(4.1)B_(2.3)V_1 Alloys

The natural passive films forrned on Fe_(40)Ni_(40)P_(14)B_6 and Fe_(54.6)Ni_(38)Si_(4.1)B_(2.3)V_1 amorphous alloys long-term exposed in air have been studied by X-ray photoelectron spectroscopy (XPS) and Auger electron (including Ar+ ion depth profiling) spectroscopy (AES). The following aspects have been investigated: (1) chemical states of the elements in the films. binding energies and the chemical shifts measured by XPSf (2) structure and composition of the films fand (3) thickness of the passive films determined by AES depth profiling and XPS analysis.     

共沉淀法合成La_(0.9)Sr_(0.1)Ga_(0.8)Mg_(0.2)O_(3-δ)及其性质的研究

采用共沉淀法合成了具有钙钛矿结构的中温固体电解质La_(0.9)Sr_(0.1)Ga_(0.8)Mg_(0.2)O_(3-δ)(LSGM),并用DTA-TGA和X射线衍射仪分析了LSGM材料中钙钛矿相的形成过程,采用SEM、交流阻抗谱等检测技术对LSGM电解质的结构及性能进行了表征.XRD分析结果表明,1200℃烧结后,粉体开始形成钙钛矿结构,随温度的升高粉体中杂相含量越来越少,于1450℃时形成了单一的钙钛矿相结构.