16 resultados para BATIO3

em Chinese Academy of Sciences Institutional Repositories Grid Portal


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X-ray photoelectron spectroscopy has been used to measure the valence band offset of the ZnO/BaTiO3 heterojunction grown by metal-organic chemical vapor deposition. The valence band offset (VBO) is determined to be 0.48 +/- 0.09 eV, and the conduction band offset (CBO) is deduced to be about 0.75 eV using the band gap of 3.1 eV for bulk BaTiO3. It indicates that a type-II band alignment forms at the interface, in which the valence and conduction bands of ZnO are concomitantly higher than those of BaTiO3. The accurate determination of VBO and CBO is important for use of semiconductor/ferroelectric heterojunction multifunctional devices.

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于2010-11-23批量导入

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La2Zr2O7 (LZ) is a promising thermal barrier coating material for the high-temperature applications, which could be significantly toughened by the BaTiO3 piezoelectric phase incorporated into the matrix. The composites of xBaTiO(3)/(l-x)LZ (x=5, 10, 15, 20 vol%, LZ-x-BaTiO3) were densified by means of high-pressure sintering (HPS) under a pressure of 4.5 GPa at 1450 degrees C for 10 min, by which a high relative density above 93% could be obtained.

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Barium titanate (BaTiO3) powders with particle sizes of 30 similar to 50 nm were prepared from barium stearate, titanium alkoxides and stearic acid by stearic acid-gel method. Dispersing the agglomerate of BaTiO3 nanoparticles into poly(amic acid) solution followed by curing led to the formation of polyimide hybrid films. The hybrid films were transparent and well distributed with BaTiO3 nanoparticles when the BaTiO3 content was less than 1 wt%. Highly loaded hybrid film containing 30 wit % BaTiO3 was tough, had a smooth surface and possessed much higher dielectric and piezoelectric constants than the parent polyimide.

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Two-step phase transition model, displacive to order-disorder, is proposed. The driving forces for these two transitions are fundamentally different. The displacive phase transition is one type of the structural phase transitions. We clearly define the structural phase transition as the symmetry broking of the unit cell and the electric dipole starts to form in the unit cell. Then the dipole-dipole interaction takes place as soon as the dipoles in unit cells are formed. We believe that the dipole-dipole interaction may cause an order-disorder phase transition following the displacive phase transition. Both structural and order-disorder phase transition can be first-order or second-order or in between. We found that the structural transition temperatures can be lower or equal or higher than the order-disorder transition temperature. The para-ferroelectric phase transition is the combination of the displacive and order-disorder phase transitions. It generates a variety of transition configurations along with confusions. In this paper, we discuss all these configurations using our displacive to order-disorder two-step phase transition model and clarified all the confusions.

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La2Zr2O7是一种近年来才提出的新型热障涂层材料,该材料熔点高,在熔点以下不发生相变,热导率低,抗烧结及没有氧传输发生,这些特点使得它作为一种高温下应用的热障涂层材料越来越引起人们的重视。但是,由于该材料的热膨胀系数和断裂韧性比较低,它的实际应用受到了限制。 在本论文中,使用高压烧结的方法获得了致密化的纳米La2Zr2O7块体材料,并对其断裂韧性和热膨胀系数进行了研究。得到的La2Zr2O7纳米材料的断裂韧性和热膨胀系数分别为1.98MPam1/2和9.6×10-6K-1 (200-1000℃),这些数值明显高于非纳米的La2Zr2O7陶瓷(断裂韧性和热膨胀系数分别为1.40 MPam1/2 和 9.1×10-6 K-1,该结果表明纳米化是一种提高材料断裂韧性和热膨胀系数的有效方法。在La2Zr2O7纳米粉末中加入8YSZ纳米颗粒,高压烧结后使其颗粒充分生长,在得到的复相化合物中观察到形成了类似棒状晶体的自增韧相,使得复合材料的断裂韧性(1.88 MPam1/2)比La2Zr2O7有所提高,甚至超过了同样条件下制备的8YSZ样品的断裂韧性。 La2Zr2O7的断裂韧性也可以通过在基体中添加BaTiO3铁电材料得到明显的提高。当添加BaTiO3的体积含量达到10vol%时,4.5GPa,1450℃高压烧结10min得到的复合材料断裂韧性达1.98 MPam1/2,明显高于同条件下烧结的La2Zr2O7 (1.60MPam1/2)。应力诱导下BaTiO3的电畴转向是主要的增韧原因。随着BaTiO3颗粒添加的体积含量增加,复相化合物的热膨胀系数也明显提高。当掺杂20vol%BaTiO3时,得到的复合材料平均热膨胀系数达到10.2×10-6K-1 (150~1200℃)。 我们通过在4.5GPa, 1650℃高压烧结5min的方法还获得了掺杂YAG纳米颗粒的La2Zr2O7纳米复相陶瓷。在室温下测量了材料的维氏硬度,并通过压痕裂纹长度计算出了材料的断裂韧性。随着YAG纳米颗粒体积含量的增加,纳米复相陶瓷的断裂韧性和维氏硬度都依次增加,当添加20vol%的YAG纳米颗粒时达到最大,分别为1.93 MPam1/2和11.45GPa。断裂韧性增加的机理可归结为以下三点:一是YAG纳米颗粒的添加提高了La2Zr2O7基体的晶界强度,二是基体晶粒尺寸变化的影响,三是YAG纳米颗粒对裂纹的偏转和钉扎作用。添加微米YAG颗粒的复相化合物因为和纳米复相陶瓷具有不同的增韧机制,因此断裂韧性的变化趋势也不相同,在掺入10vol%的YAG微米颗粒时,复合材料的断裂韧性最大,而后降低,当掺入YAG微米粒子的体积含量达到20vol%时,断裂韧性甚至低于La2Zr2O7。 从20世纪90年代开始,电纺作为一种合成纤维的办法越来越吸引人们的注意。其合成的纤维长度长,直径均匀,并且组成范围很广。最初,电纺只是被用来合成一些有机聚合物的纤维,最近,很多研究组开始致力于使用电纺的方法合成复合纤维或者陶瓷纤维。 在本论文中,我们使用电纺的方法获得了La2Zr2O7纳米纤维和SiC单晶纳米线。1000℃煅烧得到的La2Zr2O7纳米纤维具有烧绿石结构,直径在200~500nm之间。同样的温度煅烧时得到的La2Zr2O7纳米纤维的比表面积要明显高于粉末样品的,表明纤维的抗烧结性能比粉末的高。得到的SiC纳米线直径在50~100nm之间,表面有一约5nm厚的无定形的SiO2薄层。 使用电纺的方法,恰当的控制煅烧条件,我们获得了La2Ce2O7, La2(Zr0.745Ce0.386)2O7.524和8YSZ中空纤维。这种中空结构减小了粒子之间的接触面积,提高了材料的抗烧结性能。在扫描电镜分析的基础上,我们总结了这些中空纤维的形成过程。

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The electronic structure of a microporous titanosilicate framework, ETS-10 is calculated by means of a first-principles self-consistent method. It is shown that without the inclusion of the alkali atoms whose positions in the framework are unknown, ETS-10 is an electron deficient system with 32 electrons per unit cell missing at the top of an otherwise semiconductor-like band structure. The calculated density of slates are resolved into partial components. It is shown that the states of the missing electrons primarily originate from the Ti-O bond. The local density of states of the Ti-3d orbitals in the ETS-10 framework is quite different from the perovskite BaTiO3. The possibilities of ETS-10 crystal being ferroelectric or having other interesting properties are discussed.

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Polyimide hybrid films containing bimetalic compounds were obtained by codoping poly(amic acid) with a barium and titanium precursor prepared from BaCO3, Ti(OBu)(4), and lactic acid followed by casting and thermal curing. FTIR, WAXD, and XPS measurements showed that barium and titanium precursor could be transformed to BaTiO3 at a temperature above 650 degreesC, while the mixed oxides were only found in hybrid films. The measurements of TEM and AFM indicated a homogeneous distribution of inorganic phase with particle sizes less than 50 nm. The hybrid films exhibited fairly high thermal stability, good optical transparency, and promising mechanical properties. The incorporation of 10 wt % barium and titanium oxide lowered surface and volume electrical resistivity by 2 and 5 orders, respectively, increasing dielectric constant from 3.5 to 4.2 and piezoelectric constant from 3.8 to 5.2 x 10(-12) c/N, relative to the nondoped polyimide film.