耐蚀合金Al3Ni和Ni3Al液态冷凝过程的比较研究

采用F S多体势对液态合金Al3Ni和Ni3Al在不同冷却速度下的微观结构及其转变机制进行了分子动力学模拟 ,得到了不同冷速下各温度的双体分布函数 ;采用HA键型指数法对其结构进行了分析 ,结果表明 :Al3Ni在两种冷速下均以非晶的形式出现 ,只是慢冷时体系的有序度略有升高 ;而Ni3Al的结构及能量转变受冷速影响较大 ,快冷时形成非晶 ,而慢冷时出现明显结晶 ;同样冷速下Al含量较少的Ni3Al体系的有序度高 ,更易形成晶体 ,晶体的形成过程中有能量突变 .     

KNO3／Al2O3和K2CO3／Al2O3的强碱性研究

采用ＣＯ２－ＴＰＤ及Ｈａｍｍｅｔｔ批示剂法测定了ＫＮＯ３／Ａｌ２Ｏ３及Ｋ２ＣＯ３／Ａｌ２Ｏ３样品的碱量和碱强度。当ＫＮＯ３，Ｋ２ＣＯ３的负载量低于其单层分散阈值时，能在ＡｌＯ３均匀分布并产生强度为１８．４的强碱位；高于其单层分散阈值后则能生成强度为２７．０的超强碱位。     

Al3O3N纳米线的制备与表征

在H2+Ar混合气氛中加入少许N2+O2气氛,采用直流电弧等离子体法制备了Al3O3N纳米线.用XRD,SEM,TEM,HRTEM测定了纳米线的成分、形貌特征、显微结构等.Al3O3N纳米线直径分布为25-110 nm,长度达5.5μm.Al3O3N纳米线是尖晶石结构.另外,对Al3O3N纳米线的生长机理进行了研究.     

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基于Mie散射理论和方法,研究了航天器尾喷焰等离子体中Al2O3粒子的光学散射特性,分析了复折射率对单个Al2O3粒子消光效率因子、散射效率因子、吸收效率因子、散射相函数以及单次反照率的影响。同时,基于多分散系粒子尺度单峰分布,分析了Al2O3粒子按粒径分布后散射场的有关效应因子及散射相函数的变化,并进行了相应的数值模拟。理论和数值模拟研究表明,航天器尾喷焰等离子体Al2O3粒子复折射率的虚部和实部、粒径的大小与分布对其散射相函数、消光和散射效率因子以及单次反照率均有明显的影响。     

Al/Al_2O_3/Al隧道结相位扩散的现象

超导约瑟夫森结是超导量子比特的核心元件,由约瑟夫森结组成的直流超导量子干涉器(DC-SQUID)由于其具有较高的探磁灵敏度,在超导磁通量子比特量子位测量中具有重要的作用.我们用铝为超导材料,采用电子束斜蒸发及静态氧化的方法制备了由两个Al/Al2O3/Al隧道结并联组成的DC-SQUID样品.将DC-SQUID样品置于20~1000mK范围内的不同温度下,对其跳变电流分布进行了测量.在50mK明显观测到了隧道结跳变电流机制由宏观量子隧穿到热激发的转变,并且在高于80mK时,观测到了相位扩散的现象.这对于隧道结相位动力学研究具有重要意义.     

Al 3p电子的L-S耦合近似计算

用Nd :YAG脉冲激光器发出的脉冲激光束烧蚀金属Al靶产生Al等离子体。利用时 空分辨技术 ,采集Al等离子体发光信息 ,获得Al原子特征辐射谱。对Al 3p电子的L S耦合进行了类氢粒子的简化处理 ,并用量子力学的相关知识详细地计算了主量子数屏蔽系数α和轨道角动量量子数屏蔽系数s。     

套管法Nb_3Al前驱线中Nb/Al界面扩散反应过程

利用套管法制备了Nb-Al七芯前驱体线材,并通过等温热处理的方式分别在700~1500℃对其进行热处理,研究了Nb-Al二元体系在其界面处的反应成相过程.研究发现700℃热处理的样品在其界面处只形成了NbAl3反应层;800~900℃热处理的样品界面处又形成一层Nb:Al≈1:1新反应层;随着热处理温度的增加到1000℃,界面处出现Nb2Al反应层,并随热处理温度的增加Nb2Al反应层的厚度增加;1400℃和1500℃热处理的样品中开始观察到了少量的Nb3Al相,磁性测量表明1400℃和1500℃条件下热处理样品的起始超导转变温度分别为14K和15.8K,说明套管法制备的Nb-Al前驱体线材在1400℃以上热处理可以获得Nb3Al超导相,但由于Nb3Al相中的Al含量偏离理想化学计量比,导致其超导转变温度偏低.     

Y3Al5O12:Ce3+,Cr3+和Y3Al5O12:Ce3+,pr3+,Cr3+荧光粉体系中的能量传递

通过在YAG:Ce3+和YAG:Ce3+,pr3+荧光粉体系中分别掺入Cr3+离子来提高蓝光管芯白光LED的显色指数.Cr3+离子的加入,增加了红光发射,这归因于Cr3+的2E-4 A2跃迁的零声子线和声子边带发光.Ce3+→Cr3+的能量传递是增强红光发射的重要方式,在YAG:Ce3+,Cr3+体系中,由发射光谱得到...     

A computational study of the electron detachment energies of Al2As2 − and Al3As3 −

Ab initio and density functional theory calculations are reported for the low-lying electronic states of Al₂As₂ ^?, Al₂As₂, Al₃As₃ ^?, and Al₃As₃. The ²B_2g ground electronic state of Al₂As₂ ^? has a rhombic structure with the Al atoms occupying the shorter diagonal. In contrast, the As atoms occupy the shorter diagonal of the ground state rhombic structure of Al₂As₂. Electron detachment energies computed for Al₂As₂ ^? are presented and discussed. The adiabatic electron affinity of Al₂As₂ ^? is calculated to be 2.1 eV at the CCSD(T) level, using B3LYP and MP2 optimized geometries. The ground states of both Al₃As₃ ^? (²A₁′) and Al₃As₃ (¹A₁′) have planar hexagonal D_3h geometry. Electron detachment energies computed for the anion are reported. At the CCSD(T)//B3LYP level, the electron affinity of Al₃As₃ is calculated to be 2.47 eV.     

高能球磨法制备Nb_3Al超导体

利用高能球磨法制备Nb_3Al超导体,先通过高能球磨法获得Nb(Al)固溶体,然后在不超过1000℃的温度下烧结将Nb(Al)固溶体转变为Nb_3Al超导相,对其成相反应过程展开研究.研究发现高能球磨法能够获得Nb(Al)固溶体,球磨3小时为宜,时间较短不能完全形成固溶体,时间较长使原料粉末非晶化.在烧结过程中,研究了原料组分、烧结温度及时间对制得超导相性能的影响,最终获得初始原料的化学计量比为Nb∶Al=74∶26、烧结温度为900℃、烧结时间为1小时制得的Nb_3Al超导体的Tc最高,达到15.6K.由于Nb_3Al相中的Al含量偏低,导致其Tc偏低.     

Superconductivity and magnetic properties of Nb—Al phases: Nb2Al and NbAl3

Magnetic properties of tetragonal phases in Nb—Al system have been investigated down to 0.42°K. It has been found that the-phase (Nb₂Al) and the intermetallic compound NbAl₃ are superconductors with superconducting transition temperature 0.74°K and 0.64°K, respectively. Magnetic susceptibility of the investigated phases does not depend on temperature within the range 4.2°K–300°K, and is equal =(1.0±0.1) × 10^–6 emu)/g for Nb₂Al, and =(0.9±0.03) × 10^–6 emu/g for NbAl₃.On leave of absence from Institute for Solid State Physics of Bulgarian Academy of Sciences, Sofia, Bulgaria     

Hybrid Al + Al3Ni metallic foams synthesized in situ via laser engineered net shaping

A hybrid, Al?+?Al₃Ni metallic foam was synthesized in situ via laser engineered net shaping (LENS®) of Ni-coated 6061 Al powder in the absence of a foaming agent. During LENS® processing, the Ni coating reacted with the Al matrix, resulting in the simultaneous formation of a fine dispersion of Al₃Ni, and a high volume fraction of porosity. As a reinforcement phase, the intermetallic compound formed particles with a size range of 1–5?µm and a volume fraction of 63%, with accompanying 35–300?µm pores with a 60% volume fraction. The microstructure of the as-deposited Al?+?Al₃Ni composite foams was characterized using SEM, EDS, XRD and TEM/HRTEM techniques. The evolution of the microstructure was analyzed on the basis of the thermal field present during deposition, paying particular attention to the thermodynamics of the Al₃Ni intermetallic compound formation as well as discussing the mechanisms that may be responsible for the observed porosity. The mechanical behavior of the as-deposited material was characterized using compression and microhardness testing, indicating that the yield strength and hardness are 190?MPa and 320 HV, respectively, which represents an increase of over three times higher than that of annealed Al6061, or similar to heat-treated Al6061 fully dense matrix, and much higher than those of traditional Al alloy foams, and with a low density of 1.64?g/m³.     

Cd3Al2Si3O12玻璃中Er3+的光学跃迁

根据Judd-Ofelt理论,利用镉铝硅酸盐玻璃中E,+的吸收光谱,计算了实验与理论振子强度,用最小二乘法拟合实验与理论振子强度得到了三个J-O强度参数Ω2,Ω4,Ω6.并由此计算了Er3+在不同能级之间的自发辐射系数A、辐射寿命ι、荧光分支比β以及积分发射截面∑.根据这些参数分析认为掺铒镉铝硅酸盐玻璃可能实现近红外激光输出.     

Simple identification of Al2O3 and MgO·Al2O3 spinel inclusions in steel using X-ray-excited optical luminescence

Nonmetallic inclusions in steel cause problems in steel products and steel production. In particular, an analysis of Al₂O₃ and MgO·Al₂O₃ spinel inclusions is important since they are one of the most harmful inclusions. A rapid and simple analysis of nonmetallic inclusions is required as the conventional analytical methods for nonmetallic inclusions are time-consuming. In this study, we propose a simple method to identify Al₂O₃ and MgO·Al₂O₃ spinel inclusions in steels. X-ray-excited optical luminescence (XEOL) analysis was selected as a promising method because it can rapidly identify sizes, shapes, and compositions of nonmetallic inclusions and can be performed in air. A model steel sample prepared by heating a mixture of Fe, Al, and MgO powders at 1550°C in argon atmosphere was used. XEOL images of the model steel sample showed that Al₂O₃ inclusions emitted blue and red luminescences. Using a filter attached to the camera, blocking light in the wavelength region above 650 nm, only the blue luminescence of the Al₂O₃ inclusions was observed. This was implemented as the luminescences of the Al₂O₃ inclusions appeared in both blue and red regions at wavelengths of 350, 485, 695, and 750 nm; consequently, the luminescences at 695 nm and 750 nm were blocked by the filter. In contrast, MgO·Al₂O₃ spinel inclusions emitted green luminescence (peak at 520 nm), unaffected by the filter. This indicates that we can simply identify Al₂O₃ and MgO·Al₂O₃ spinel inclusions by an XEOL image in the wavelength range of 420–650 nm.     

μSR studies in the heavy fermion systems UNi2Al3, UPd2Al3 and U2PtC2

We have performed Muon Spin Relaxation (SR) measurements of several heavy fermion systems: UNi₂Al₃ (single crystal), UPd₂Al₃ (single crystal) and U₂PtC₂ (polycrystal). ZF -SR measurements of UNi₂Al₃ show magnetic order below the Néel temperatureT _N=4.6K, with the muon precession frequency(T 0)=2.5MHz at low temperatures. The local field distribution obtained at low temperatures in UNi₂Al₃ resembles that of the incommensurate spin density wave (SDW) system (TMTSF)₂PF₆, suggesting an incommensurate spin arrangement in UNi₂Al₃. TF -SR measurements give the penetration depth(T 0)=6100Å for UPd₂Al₃ and(T 0)=7000Å for U₂PtC₂ respectively. Since UPd₂Al₃ and U₂PtC₂ are clean superconductors (/l-0), we can combine n _s/m^* with the Sommerfeld constant n _s ^1/3 m^* to calculate the Fermi temperatureT _F ^3/4–1/4, which represents the characteristic energy scale of the superconducting carriers. We obtainT _C/T_F 0.01 for both UPd₂Al₃ and U₂PtC₂, comparable to other exotic superconductors, but quite different from simple metal BCS superconductors, whereT _C/T_F 0.01.     

Yb:Y3Al5O12/Y3Al5O12复合晶体的制作和光谱性能

采用热键合技术,制作中运用不同的工艺参量制作出12片Yb:Y3Al5O12/Y3Al5O12(Yb:YAG/YAG)复合.晶体.利用偏光显微镜对其键合界面进行了观察,研究了样品的透射光谱,从而确定出复合晶体合适的制作工艺.通过透射光谱的形状和透射率来表征复合晶体键合界面的质量.研究表明Yb:YAG/YAG复合晶体键合质量较好,可实现一体化.