合金元素Zr韧化不同计量比Ni3Al合金的微观机制

利用正电子湮没技术(PAT)测量了不同化学计量比二元Ni3Al合金及不同Zr含量Ni3Al合金的正电子寿命谱,并估算了合金基体和晶界缺陷处的自由电子密度.结果表明,二元Ni77Al23合金的基体和缺陷态的自由电子密度都比二元Ni74Al26合金的高.Ni3Al合金晶界缺陷处开空间大于Ni空位或Al空位的开空间,晶界缺陷处的自由电子密度很低,金属键合力很弱.过化学计量比Ni74Al26合金的晶界缺陷开空间比亚化学计量比Ni77Al23合金的大,晶界结合力更弱.这是Ni74Al26合金更脆的原因.在Ni3Al合金中加入Zr,增加了合金中的金属键成分,使基体中的自由电子密度增加,增强了基体金属键合力,同时降低了合金的有序度,使合金晶界容易弛豫,晶界缺陷的开空间变小.另外,Zr原子偏聚到晶界,增加了晶界处的自由电子密度,同时引起晶界处Al贫化,减少了强共价性Ni-Al和Al-Al键,使晶界更易于变形,有利于提高合金的塑性.     

B改善单晶和多晶Ni3Al合金力学性能的微观机制

通过测量Ｂ含量从０．００至２．２２ａｔ％的单晶和多晶Ｎｉ₃Ａｌ合金的正电子寿命谱，研究了单晶和多晶Ｎｉ₃Ａｌ合金中的微观缺陷和电子结构。结果表明，多晶Ｎｉ₃Ａｌ合金晶界中存在着开空间大于空位的缺陷。晶界缺陷处参与形成Ｎｉ－Ｎｉ和Ｎｉ－Ａｌ键的价电子浓度比基体或位错处的低，晶界是结合力弱化区域。偏聚到Ｎｉ₃Ａｌ合金缺陷上的Ｂ与缺陷处的Ｎｉ或Ａｌ原子形成强的共价键而增强了这些地方的结合力。以间隙方式固溶到Ｎｉ_{3< 关键词：}     

合金元素韧化或脆化FeAl金属间化合物的微观机制

通过测量二元FeAl以及含B，Zr或Si的FeAl合金的正电子寿命谱参数，计算合金基体和缺陷处的价电子密度.结果表明，当Al原子和Fe原子结合形成FeAl合金时，Al原子提供价电子与Fe原子的3d电子形成局域的共价键.FeAl合金基体的价电子密度很低，FeAl合金中金属键和共价键共存.FeAl合金晶界缺陷的开空间大于Fe空位或Al空位的开空间，FeAl合金晶界处的金属键合力很弱.在FeAl合金中加入少量的B，一部分B原子以间隙方式固溶到FeAl基体中，增加基体的价电子密度；另一部分B原子偏聚到FeAl合金的晶界上，也增加了晶界处的价电子密度.在FeAl合金中加入Zr，增加了合金中的金属键成分，使基体中的价电子密度增加，增强了基体中金属键合力.Zr原子的加入还降低了FeAl合金的有序度，使合金晶界容易弛豫，晶界缺陷的开空间变小.Zr原子在晶界附近出现，还增加了晶界处的价电子密度.在FeAl中加入B或Zr有利于提高合金的韧性.在FeAl合金中加入Si，晶界处的Si原子与邻近的原子形成强的共价键，使得在晶界处参与形成金属键的价电子密度降低.在FeAl中加入Si使合金更脆. 关键词：     

铬和镍的添加对Fe3Al合金力学性能影响的DFT研究

利用第一原理研究了过渡金属元素 Cr 或 Ni 在 Fe₃Al合金中的优先占位行为及其合金化效应. 计算结果表明: Cr 或 Ni 的取代有助于Fe₃Al 合金体系更稳定, Cr 优先占据 Fe_I 位, Ni 优先占据 Fe_II位. Fe₂NiAl-II 具有最小的剪切模量G, 杨氏模量E和G/B值, 因此Fe₂NiAl-II合金的韧性、延展性最佳. 态密度和电荷密度图表明, 过渡金属元素的取代提高了它们与近邻基体原子之间的相互作用, 削弱了Al和Fe的相互作用.     

Fe-Si-Al合金结构的研究

本文叙述了利用电子显微镜对含10％Si和5％Al的Fe-Si-Al高导磁合金薄膜进行的结构研究。发现了基体为有序面心立方Fe₃(Al,Si)结构,其晶格参数为5.70±0.03?,该值在Fe₃Si和Fe₃Al晶格参数之间,说明部分Si原子为Al原子所置换。并获得三套基体和析出相合成的电子衍射图,相应确定了基体和析出相的取向关系:(001)_基‖(110)_相;[100]_基‖[00I]_相;[010]_基‖[I10]_相。对析出相的萃取碳复型,在电子显微镜中进行选区衍射,获得了立方Fe₃(Al,Si)C_x相的结构。提出:Fe原子占据面心;Al或Si原子占据顶角;C原子占据体心的看法。 关键词：     

Mo,Ta, W在NixAl1-x(x=0.25,0.5,0.75) 中的择优占位

用多体势结合分子动力学计算了L1₂型NiAl₃, L1₂型Ni₃Al, L1₀型NiAl和B₂ 型NiAl的晶格常数, 结合能以及合金形成热; 分析了结构性点缺陷在上述四种合金中的存在形式; 在此基础上研究了合金化元素Mo, Ta, W在Ni_xAl_1-x(x=0.25,0.5,0.75)中的择优占位行为. 计算结果表明: 对于四种结构的Ni-Al合金, 偏离理想化学配比时,主要的结构缺陷形式是反位置; 根据占位能最小化, 第三组元元素Mo, Ta, W在上述四种Ni-Al中都显著优先占据Al格位. 关键词： 多体势 Ni-Al合金 占位     

甲脒碘化铅单晶基钙钛矿太阳能电池的研究

近年来,CH(NH₂)₂PbI₃(FAPbI₃)由于其带隙接近理想值而受到了广泛关注,成为钙钛矿太阳能电池中最具吸引力的光电功能材料.然而由碘甲脒(FAI)和碘化铅(PbI₂)作为前驱体制备的传统钙钛矿层化学计量比不精准,缺陷密度大,稳定性差且结晶度较低,导致钙钛矿太阳能电池性能很难进一步提高.本文采用FAPbI₃单晶制备的钙钛矿薄膜具有高结晶度,高稳定性,精确的化学计量比和低缺陷密度.单晶钙钛矿薄膜的晶粒尺寸大,晶界少,导致晶界处缺陷较少,提高了钙钛矿太阳能电池的短路电流密度(J_SC)和开路电压(V_OC),使其光电转换效率有了大幅度的提高.本文为制备高稳定性、高结晶度和低缺陷密度的钙钛矿太阳能电池提供了一种有效策略.     

铁基纳米晶合金的热膨胀研究

研究了铁基纳米晶合金Ｆｅ_１３．５Ｃｕ_１Ｎｂ_３Ｓｉ_１３．５Ｂ_９和Ｆｅ_９１Ｚｒ_７Ｂ_２的热膨胀特性，并与相应成分的非晶合金做了比较。结果表明，在居里温度以下，纳米晶合金的热膨胀系数比非晶合金大得多，而在居里温度以上，两者几乎相等。认为上述的热膨胀的差别可能与铁基非晶态合金中存在的因瓦效应有关。 关键词：     

镍基单晶超合金Ni/Ni3Al晶界的分子动力学模拟

在镍基单晶超合金中，由于单晶Ni的晶格常数比单晶Ni₃Al的稍小，在Ni/Ni3Al晶界面 上必然要出现错配.采用分子动力学模拟了镍基单晶超合金的Ni/Ni₃Al晶界的结 构，考虑 了两个不同的初始模型，并进行了分子动力学弛豫.弛豫的结果均表明：由于晶格的差异形 成的错配能不是通过长程晶格错配的方式来释放，而是通过在局部区域形成位错的方式释放 的.由于Ni₃Al相周围Ni相环境的不同，形成的位错也有所不同. 关键词： 镍基单晶超合金 晶界 分子动力学模拟     

非晶Ni-P合金的晶化相

利用电镜双倾台倾转Ni₁₂P₅晶体以及对Vafaei-Makhsoos发表的数据的分析,证实了由他所提出的三个新的Ni₃P相并不存在。从而澄清了非晶Ni-P合金在加热过程中总共有七个晶化相析出:α=5.48?的面心立方亚稳相α,由此相转变生成的六角多型体α₁,α₂,α₃亚稳相,体心四方Ni₁₂P₅相,体心四方Ni₃P相及Ni固溶体。 关键词：     

Zr催化剂对NaAlH4和Na3AlH6可逆储氢性能的影响

采用基于密度泛函理论的平面波赝势方法,分别计算纯净的以及掺杂Zr的NaAlH₄和Na₃AlH₆的晶格结构常数、能量、电子局域函数和电子态密度.结果表明：NaAlH₄和Na₃AlH₆分别是带隙为46和31 eV的绝缘体;NaAlH₄和Na₃AlH₆中Al—H键是共价键,Na—H键是离子键;Zr原子替代Na原子 关键词： 储氢 4')" href="#">NaAlH₄ 3AlH₆')" href="#">Na₃AlH₆ Zr掺杂     

Free Surface and Interface Thermodynamics of Liquid Nickel in Contact with Alumina

Sessile drop experiments of Ni and Ni(2at.%Al) were conducted under controlled working conditions, at 1500°C, P(O₂) 10^–9 Torr. It is shown that Al and oxygen atoms engaged in the capillary driven mass transport at the interface have a significant impact on the surface/interface thermodynamics. The surface energy of liquid Ni determined from experiments in which Ni comes into contact with Al₂O₃ is significantly lower than that of high purity Ni, due to the segregation of Al. The free energy of segregation of Al to the free surface of Ni ( G _S) was found to range from –164 to –152 kJ/mol, indicating a relatively strong tendency for segregation of Al to the free surface of Ni(Al). It is proposed that an Al(O)-rich liquid layer forms adjacent to the Ni-Al₂O₃ interface, which improves interfacial adhesion. In the Ni(Al)-Al₂O₃ system, an increase in the Al content of the alloy leads to the improvement of both wetting and adhesion of the alloy on the ceramic, correlating with the improvement in the interface strength after solidification.     

Diffusion research between Ni3Al coating and titanium alloy produced by plasma spraying process

A Ni₃Al coating was prepared by plasma spraying technique on the surface of titanium alloy. Ni-Al mixed powders, coatings and reaction products were investigated by scanning electron microscope, EDS, DSC and XRD. A tight bonding between the coating and the substrate was formed. The X-ray diffraction analysis of the patterns showed that the coating not only had Ni₃Al phase, but also had NiO and Al₂O₃ phase microcontent. Comparing Ni coated Al to Ni₃Al at 900 °C, the diffusion was stronger and the diffusion layer was thicker. A minute pore structure was formed at 1200 °C in the front edge of solid-state reaction layer. So Ni₃Al restrained the solid-state reaction of the coating with the substrate, and as a whole weakened the entry of oxygen atoms into the substrate and quenched the out-diffusion of titanium.     

模拟锆(Zr) 的基体效应对Ni3Al-x atoms % Zr晶界内聚性的影响(英文)

利用双粒子模型研究微量元素锆(Zr)的基体效应对Ni3Al x atoms % Zr晶界内聚性的影响. 模型显示， x\[锆(Zr)的基体浓度\]从0.1增加到0.5， 在晶界Zr富集是增加的； Ni富集和Al贫乏在x=0.3时趋于最大. 模型还显示， Ni3Al x atoms % Zr晶界的内聚性在x=0.3时为最佳.     

The behavior of 3d electrons and defects in TiAl-based alloys containing V and Cu studied by positron annihilation

Information of defects and 3d electrons in transition metals (Ti, V, Cu) and TiAl-based alloys (Ti₅₀Al₅₀, Ti₅₀Al₄₈V₂, Ti₅₀Al₄₈Cu₂) can be extracted from the positron lifetime and coincidence Doppler broadening spectra. The results show that the 3d electron signals for the transition metals Ti, V and Cu increase with the number of 3d electrons. The 3d electron signal and the electron density for binary TiAl alloy are relatively low due to the (Ti)3d-(Al)3p interactions. The addition of V and Cu atoms to TiAl alloy leads to the increase in the electron densities in bulk and the defects on grain boundaries simultaneously, as well as the enhancement of the 3d electron signal. The 3d electron signal in the spectrum of Ti₅₀Al₄₈Cu₂ alloy is higher than that of Ti₅₀Al₄₈V₂ alloy.     

The Electronic Structure of Pristine and Doped (100) Tilt Grain Boundaries in SrTiO3

To understand the electronic properties of doped grain boundaries, we reviewed the atomic scale techniques currently available to study the electronic structure at pristine SrTiO₃ grain boundaries. The knowledge gained from the pristine boundaries is used to interpret experimental and theoretical results from a Mn doped 5 SrTiO₃ grain boundaries. Mn atoms are shown to preferentially substitute at specific Ti sites at the grain boundary core. Furthermore, the formal oxidation state of the Mn atoms at the grain boundary core was found to be reduced compared to the Mn atoms substituting for Ti in the bulk. This change of valence did not, however, significantly affect the atomic structure of the grain boundary, as determined by Z-contrast imaging and electron energy-loss spectroscopy, which revealed similar fine-structure features at both the doped and pristine grain boundary. We conclude, therefore, that composition and atomic structure have different effects on the local electronic structure and should be treated separately in any segregation and electrical conductivity models for grain boundaries.     

First-principles calculations for the elastic properties of Ni-base model superalloys: Ni/Ni3Al multilayers

A model system consisting of Ni[001](100)/Ni3Al[001](100) multi-layers are studied using the density functional theory in order to explore the elastic properties of single crystal Ni-based superalloys. Simulation results are consistent with the experimental observation that rafted Ni-base superalloys virtually possess a cubic symmetry. The convergence of the elastic properties with respect to the thickness of the multilayers are tested by a series of multilayers from 2γ′+2γ to 10γ′+10γ atomic layers. The elastic properties are found to vary little with the increase of the multilayer’s thickness. A Ni/Ni3Al multilayer with 10γ′+10γ atomic layers (3.54 nm) can be used to simulate the mechanical properties of Ni-base model superalloys. Our calculated elastic constants, bulk modulus, orientation-dependent shear modulus and Young’s modulus, as well as the Zener anisotropy factor are all compatible with the measured results of Ni-base model superalloys R1 and the advanced commercial superalloys TMS-26, CMSX-4 at a low temperature. The mechanical properties as a function of the γ′ phase volume fraction are calculated by varying the proportion of the γ and γ′ phase in the multilayers. Besides, the mechanical properties of two-phase Ni/Ni3Al multilayer can be well predicted by the Voigt-Reuss-Hill rule of mixtures.