Fe-C—Sb合金中液态急冷获得的ε相的分解

本工作用示差热分析法,淬火样品X射线衍射法和Guinier-Lenn透射式高温单色聚焦粉末照相法研究了Fe-C-Sb合金中液态急冷获得的ε相的高温分解过程,实验结果指出,ε相在125℃开始分解,首先分解成ε-Fe₂C,而后在450℃分解成α-Fe,并析出Sb和Fe₃Sb₂,还保留有ε-Fe₂C;在550℃以后ε-Fe₂C转变成Fe₃C,并在770℃时发生Fe的α→γ转变,在800℃时主要组成相为:γFe,Sb,Fe₃C(Fe₃Sb分解);在冷却过程中750℃发生Fe的γ→α转变,冷至室温时的主要组成相是:αFe,Fe₃C,Sb,Fe₃Sb₂。 关键词：     

Fe-C-Sb合金中液态急冷获得的ε相的高压稳定性及其相变

本工作用X射线粉末照相法研究了Fe-C-Sb合金中液态急冷获得的ε相在高压下的相变过程。实验结果表明,压力对ε相的稳定性及其相变过程都有显著影响。在4.7GPa压力下,ε相的稳定化温度提高到450℃左右,而后合金中开始出现在常压下未曾出现过的新的正交结构亚稳相。在上述压力下,当温度达到560℃时,该正交结构亚稳相开始转变成Fe₃C;在800℃时,Fe₃C分解成单质状态的石墨碳和γ-Fe,这时合金的相组成为:C,γ-Fe,Sb及另一未知相。 关键词：     

Al-Cr-Cu三元合金系相图的室温截面

本文用X射线粉末衍射法研究了Al-Cr-Cu三元合金系相图的室温截面。截面中出现了五个新相,称为ω₁,ω₂,ε_f,ε_x和γ_x,即共有19个单相区,41个双相区以及22个三相区。γ_x相属正交晶系,它可能是一个固定成分的化合物。 关键词：     

非晶态合金La72Si28晶化过程中生成的新亚稳超导相

本文报道了在非晶态合金La₇₂Si₂₈晶化过程中生成新亚稳超导相的实验结果。非晶态合金La₇₂Si₂₈是用液态急冷法制备的,该合金经250℃,30min热处理后,得到了一个新的亚稳超导相,该相具有正交结构,其晶格参数为a=9.121?,b=6.821?,c=3.833?,超导临界温度T_c为3.02K,高于目前已知的La-Si系超导相的T_c值。 关键词：     

深过冷Cu60Sn30Pb10偏晶合金的快速凝固

实现了大体积Cu₆₀Sn₃₀Pb₁₀偏晶合金的深过冷与快速凝固. 实验获得的最大过冷度为173 K(0.17T_L). 凝固组织发生了明显的宏观偏析,XRD分析表明,试样上部是由固溶体(Sn),(Pb)相和金属间化合物ε(Cu₃Sn)相组成的三相区,下部为富(Pb)相区. 在小过冷条件下,三相区中ε(Cu₃Sn)相的凝固组织为粗大的枝晶,随着过冷度的增大,ε(Cu₃Sn)相细化成层片状组织,且层片间距随过冷度的增大而减小,而(Sn),(Pb)两相始终以离异共晶的方式存在. 富(Pb)相区中分布有少量的ε(Cu₃Sn)枝晶,枝晶长度随过冷度的增大而增大,且在大过冷条件下发生碎断. (Sn)相在ε(Cu₃Sn)相表面形核、长大,其形态类似于包晶凝固组织. 关键词： 深过冷 快速凝固 偏晶合金 层片组织     

Al-Ti-V-M四元系合金TiAl3-VAl3-MAl3(M=Ni,Fe)赝三元系相图的室温截面

本文用X射线衍射法测定了Al-Ti-V-M四元系合金TiAl₃-VAl₃-MAI₃(M=Ni,Fe)两个赝三元系相图的室温截面。(1)TiAl₃-VAl₃NiAl₃赝三元系相图室温截面由一个单相点ε(NiAl₃)、一个单相区δ(TiAl₃和VAl₃形成的连续固溶体)和一个两相区δ+s所组成。(2)TiAl关键词：     

液态急冷Fe-12.6at%B合金中的六角亚稳相

本文利用X射线粉末照相法及透射电子显微镜选区电子衍射法,唯一地确定了作者在液态急冷Fe-12.6at％B合金中发现的新亚稳相具有六角点阵。其点阵参数为α=5.501? c=7.213?,c/α=1.311。 关键词：     

铸锭凝固组织对相应非晶合金晶化过程中二十面体准晶相形成动力学的影响

通过在真空电弧熔炼炉内对合金铸锭进行反复熔炼处理，获得到了凝固组织不同的Zr₆₅Al_7.5Cu_12.5Ni₁₀Ag₅合金铸锭.在相同的制备条件下，由凝固组织不同的合金铸锭通过吸铸法制备得到了薄片非晶合金.利用差示扫描量热法(DSC)对非晶合金的晶化动力学进行了分析.x射线衍射谱表明，在Zr₆₅Al_7.5Cu_12.5Ni₁₀Ag₅非晶合金晶化过程中，二十面体准晶相(I相)作为初生相析出.Kissinger分析结果表明，合金铸锭的凝固组织细化，相对应的非晶合金发生晶化时，I相形成与分解的有效激活能都增大，说明非晶合金及析出的I相的热稳定性都提高.从结构的遗传性角度就合金铸锭凝固组织对相应非晶合金晶化过程中二十面体准晶相的形成动力学的影响进行了讨论. 关键词： 二十面体准晶相 晶化动力学 凝固组织     

铁冲击相变的分子动力学研究

用分子动力学方法模拟了单晶铁(Fe)在一定初始温度下冲击相变(α相→ε相)的微观过程，结果显示温度会导致冲击相变压力阈值降低.基于此微观过程，对加卸载波系的传播规律进行了相应计算和分析，结果表明在卸载过程中逆相变波(ε相→α相)相对于波前以当地纵波声速传播，而相对波后以亚声速传播，这可由卸载压力-密度曲线给出相应解释；计算了不同初态的卸载压力-密度状态曲线，并给出了逆相变带的分布，其分布规律显示了卸载过程逆相变的滞后现象. 关键词： 分子动力学 多体势 冲击波 相变     

镁基合金自由枝晶生长的相场模拟研究

利用定量相场模型, 以Mg-0.5 wt.%Al合金为例模拟了基面((0001)面)内镁基合金的等温自由枝晶生长过程. 通过研究该合金体系数值模拟的收敛性, 获得了最优化值耦合参数λ = 5.5及网格宽度Δx/W₀ = 0.4, 并在该参数下系统研究了各向异性强度和过饱和度对枝晶尖端生长速度、尖端曲率半径、Péclet数及稳定性常数σ^* 的影响. 结果表明, 由微观可解性理论得到的稳定性系数σ^* 与ε₆ 拟合值σ^*≅ ε₆ ^1.81905, 更接近理想值σ ^* (ε₆) ≅ε₆ ^1.75. 此外, 当过饱和度Ω < 0.6时, 稳定性系数σ ^* 不随ε₆ 的变化而变化, 而当Ω > 0.6时, 稳定性系数σ ^* 随着ε₆ 的增加而减小. 这反映了枝晶的生长由扩散控制向动力学控制的转变. 随着过饱和度的增加, 枝晶形貌由雪花状枝晶向圆状枝晶转变.     

Crystalline Sb–Cu alloy films as anode materials for Li-ion rechargeable batteries

A crystalline Sb–Cu alloy is investigated for use in Li-ion rechargeable batteries, and its structural, electrochemical and thermal properties are characterized. A pulse electrodeposition method is used to prepare Sb–Cu alloy film on Cu foil as a negative electrode. The structure of the alloy film electrode is characterized using XRD, FE-SEM and EDX. The electrochemical behavior of the Sb–Cu alloy film is investigated at the current rate of 0.1C to the cut-off potential range of 1.8 and 0.01 V vs. Li/Li⁺. Our experimental results demonstrate that the initial discharge capacity is 850 mAh g^?1 and that the discharge capacity increases to 1034 mAh g^?1 at the end of the 30th cycle with a stable cycle life. The Coulombic efficiency is approximately 83.5% with good cyclability. Moreover, the crystalline Sb–Cu alloy film has relatively low exothermic properties, and it may be an interesting candidate for use in the negative electrodes of Li-ion batteries.     

α-LiIO3的等温压缩和高温高压下的相变

用金刚石压砧高压X射线衍射技术研究了α-LilO₃在室温高压下的压缩行为,压力达23.0GP_a。观察到晶格压缩的各向异性,其c/a轴比以-6.187×10^-3/GP_a的速率减小。得到其常压下的体弹模量B₀=39.2GP_a,体弹模量对压力的一阶导数B＇₀=3.787。α-LiIO₃在高温高压下转变成四方结构,与淬火卸压所得的ε-LiIO₃结构一致。 关键词：     

Dopant activation in Sb-implanted relaxed Si1−xGex alloy layers grown on compositionally graded buffers

Supersaturated solid solutions of substitutional, electrically active Sb have been obtained by ion implantation of relaxed epitaxial Si_1?xGe_x alloy layers grown on compositionally graded buffers. Substitutional and nonsubstitutional Sb fractions in relaxed Si_0.85Ge_0.15, Si_0.65Ge_0.35 and Si_0.50Ge_0.50 alloy layers implanted to a dose of 5×10¹⁵ Sb cm^?2 and annealed isothermally at temperatures ranging from 400 to 850°C have been studied by Rutherford backscattering/channeling, transmission electron microscopy and Hall-effect and sheet resistivity measurements. A supersaturated solution of Sb corresponding to a peak carrier concentration of 4×10²⁰ cm^?3 and an electrically active fraction of 40% of the implanted dose is observed by Hall measurements for the case of Si_0.85Ge_0.15 and Si_0.65Ge_0.35 alloys annealed at 550°C.     

Graphene Nanosheets Suppress the Growth of Sb Nanoparticles in an Sb/C Nanocomposite to Achieve Fast Na Storage

Presently, graphene incorporation is one of the most effective strategies to develop superior electrode materials for sodium‐ion batteries (SIBs). Herein, it is excitingly found that an incorporated graphene nanosheet in the preparation processes can not only completely protect all the Sb nanoparticles in an Sb/C composite from being inactivated, but also suppresses their growth to undesirable micrometer size. While there are still many exposed Sb particulates on the surface of pristine Sb/C microplates, the graphene‐incorporated Sb/C/G nanocomposite consists of uniform Sb nanoparticles of 20–50 nm, all of which have been protected by and wrapped in the mixed carbon network. When used as anode materials for SIBs, the Sb/C/G nanocomposite exhibits the best Na‐storage properties in terms of the highest reversible capacity (650 mA h g^?1 at 0.025 A g^?1), fastest Na‐storage ability (290 mA h g^?1 at a high current density of 8 A g^?1), and optimal cycling performance (no capacity decay after 200 cycles), in comparison to pristine Sb/C and pure Sb. It is further revealed that the much enhanced performance should originate from the improvement of Na‐storage kinetics and increase of electronic conductivity via comparing the electrochemical impedance spectra, and cyclic voltammetry profiles, as well as the polarization variation along with current densities.     

机械合金化合成CoSb3过程中的固相反应机理的热力学解释

用Co和Sb作为初始原料，通过机械合金化(mechanical alloying, MA)的方法合成了CoSb₃,并系统研究了MA转速和MA时间对MA过程中固相反应的影响.XRD结果表明，相同MA转速下，CoSb₃的量随MA时间的延长而增多，但是MA时间过长会导致大量CoSb₂的生成，甚至诱发CoSb₃分解为CoSb₂和非晶态Sb.而提高MA转速，只能缩短固相反应的发生时间，而不会改变整个固相反应 关键词： 机械合金化 热电材料 3')" href="#">CoSb₃ 非平衡热力学     

Effect of buffer layers on the property of Pb(Zr,Ti)O3-Pb(Mn,W,Sb,Nb)O3 thin films grown by pulsed laser deposition

New ferroelectric Pb(Zr,Ti)O₃-Pb(Mn,W,Sb,Nb)O₃ (PZT-PMWSN) thin film has been deposited on a Pt/Ti/SiO₂/Si substrate by pulsed laser deposition. Buffer layer was adopted between film and substrate to improve the ferroelectric properties of PZT-PMWSN films. Effect of a Pb(Zr_0.52Ti_0.48)O₃ (PZT) and (Pb_0.72La_0.28)Ti_0.93O₃ (PLT) buffer layers on the stabilization of perovskite phase and the suppression of pyrochlore phase has been examined. Role of buffer layers was investigated depending on different types of buffer layer and thickness. The PZT-PMWSN thin films with buffer layer have higher remnant polarization and switching polarization values by suppressing pyrochlore phase formation. The remnant polarization, saturation polarization, coercive field and relative dielectric constant of 10-nm-thick PLT buffered PZT-PMWSN thin film with no pyrochlore phase were observed to be about 18.523 μC/cm², 47.538 μC/cm², 63.901 kV/cm and 854, respectively.     

急冷Al80Mn20合金准晶T相的晶化动力学

本文研究了急冷Al₈₀Mn₂₀合金准晶T相的晶化过程。DSC实验证实在晶化过程中激活能保持不变,从而得到了晶化转变机理实验曲线,并确定了晶化激活能和频率因子的数值,它们分别为224kJ/mol和1.2×10¹²s^-1。分析结果表明准晶T相的晶化是由长程扩散所控制的,并在晶化过程中没有显著的新核形成。 关键词：