The synthesis of polycrystalline H3O+β″βAl2O3 ceramics from conventional precursor NaKβ″/βAl2O3 powders

H₃O⁺β″Al₂O₃, H₃O⁺/βAl₂O₃ and H₃O⁺β″/βAl₂O₃ /ZrO₂ ceramics of equiaxed, fine-grained microstructure were prepared by conventional synthesis techniques, gas-phase and vapour-phase ion exchange to the potassium form and field-assisted ion exchange in dilute HCl vapour to the hydronium form. The bend strength of the polycrystalline H₃O⁺β″Al₂O₃ and H₃O⁺β″/βAl₂O₃ was > 200 MPa. The conductivity of H₃O⁺β″Al₂O₃, H₃O⁺β″/βAl₂O₃ ZrO₂ was 8×10⁻⁶, 2×10⁻⁶ and 9×10⁻⁷ (Ω cm)⁻¹, respectively, at 25°C. The materials were demonstrated to perform in steam electrolysis cells at 100°C.     

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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。     

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。     

Al2O3衬底上生长的40.2K转变温度的MgB2厚膜

我们采用混合物理化学气象沉积方法(简称HPCVD)方法在(0001)晶向的Al2O3衬底上成功的沉积了1.3微米厚的MgB2超导厚膜.电性测量表明这种厚膜具有40.2K的超导转变温度,转变宽度为0.15K,绝对零度时Hc2(0)为13.7T,同时剩余电阻率达到RRR=11.磁性测量表明这种厚膜在5K和零场的条件下具有5×106A/cm3的高临界电流密度.     

Conduction mechanism in Na+ β-Al2O3

Potential calculations using Coulomb, short-range repulsive and polarization terms have been performed using Wang's method combined with the Busing WMIN version in order to analyze different collective in-phase modes of conductivity in Na⁺ β-Al₂O₃. It is concluded that among the various modes, the interstitialcy like caterpillar mechanism is the most favourable for conductivity and that the formation of pairs of Na⁺ is favoured by the polarization energy. A critical review of some conductivity mechanisms is made. Among the three categories of Na⁺ ions which are reported, at 300 K, two have a residence time shorter than 5 × 10⁻¹⁰ s. These results are compared with Raman and quasi elastic neutron results.     

Al替代对β-Ga2 O3∶Cr3＋结构与发光性能影响

高温固相法制备了（Ga1- x Alx ）2 O3∶Cr3＋（x＝0,0.1,0.2,0.3,0.4,0.5）系列荧光粉。X射线衍射分析表明Al3＋含量增加后,物相依然保持β-Ga2 O3的相。此外随着Al离子含量的逐渐增加,高衍射角峰位向右移动表明Al离子进入了β-Ga2 O3晶格中。激发光谱中258,300,410和550 nm左右的峰位分别对应基质Ga2 O3的带与带的吸收跃迁、电荷迁移带跃迁、Cr3＋的4 A2→4 T1以及4 A2→4 T2跃迁。随着Al离子掺杂量的增加,激发光谱峰位都呈现出不同程度的蓝移现象,这分别是由于基质的带隙能量、C r3＋与配体之间的电负性以及晶场强度增大所导致的。在发射光谱中,随着Al3＋替代Ga3＋,Cr3＋的发光由宽带发射变为窄带发射,这是由于Al3＋的掺入改变了Cr3＋周围的晶场,从而Cr3＋的红光发射由原来的4 T2→4 A2变为2 E→4 A2跃迁发射。Al离子掺杂改善了样品的长余辉发光特性,并且Al离子含量达到0.5时显示出较长时间的肉眼可见的近红外余辉发射。热释发光曲线显示材料中具有合适的陷阱能级,这也是材料产生长余辉发光的原因。     

氧化态K—MoO3／γ—Al2O3催化剂结构的EXAFS研究

对Ｎａ２ＭｏＯ４．２Ｈ２Ｏ，ＭｏＯ３，（ＮＨ４）６Ｍｏ７Ｏ２４．４Ｈ２Ｏ等结构典型的含钼化合物及氧化态Ｋ－ＭｏＯ３／γ－Ａｌ２Ｏ３催化剂样品进行了ＥＸＡＦＳ测试，并以Ｎａ２ＭｏＯ４．２Ｈ２Ｏ为标样进行多层拟合计算，以研究各样品钼组分的配位结构。     

Relaxation phenomena in Cr3+ doped Al2O3−Fe 2 57 O3 systems

Mössbauer absorption spectra have been measured for Cr³⁺ doped Al₂O₃?Fe ₂ ⁵⁷ O₃ systems for different values of the Cr³⁺ concentration at room temperature. The cross relaxation between Fe³⁺ and Cr³⁺ ions, which destroys the paramagnetic hyperfine structure of Fe⁵⁷ observed in undoped Al₂O₃?Fe ₂ ⁵⁷ O₃, is thoroughly studied. The experimental results suggest a new kind of cross-relaxation process involving three spins, i.e. two Fe³⁺.ions and one Cr³⁺. The process, though it is a higher-order one, is highly effective because it is energy-conserving.     

Photoluminescence quenching in zinc oxide modified by Al2O3 and Al2O3 · CeO2 Nanopowders under proton irradiations

The photoluminescence spectra of initial ZnO powder and that modified by Al₂O₃, Al₂O₃ · CeO₂ nanopowders are investigated in the range 360–660 nm before and after 100-keV proton irradiation. It is found that the introduction of nanoparticles causes a decrease in the UV-band intensity and a change in the luminescence bands in the visual spectrum due to V _O ⁺ oxygen vacancies, O _int ^- interstitial oxygen, and V _Zn ^- zinc vacancies. Luminescence quenching in the UV and visible spectra occurs under the effect of protons. The decomposition of the spectra into elementary defects and analysis of changes in their integrated intensity during modification and irradiation of the powders are carried out.     

光学晶体CsLiB6O10与K2Al2B2O7混频性能研究

基于非线性光学晶体的混频理论，利用CsLiB6O10（CLBO）晶体和K2Al2B2O7（KABO）晶体获得了紫外相干光源，详细比较了两种晶体在Ⅰ类相位匹配下的混频性能，包括混频相位匹配角、有效非线性系数、光波走离角、允许角和允许波长等参量．结果表明，KABO晶体比CLBO晶体的有效非线性系数小，其它性能均与CLBO晶体接近．这对于两种晶体用于产生紫外激光的实验研究提供了重要的理论依据．考虑到KABO晶体较好的物化性质以及不潮解这一显著特征，KABO晶体可能是最有希望实现实用化的紫外混频晶体．     

ICP-AES同时测定铬质引流剂中的Cr2O3、Al2O3、Fe2O3和MgO

探讨了电感耦合等离子体-原子发射光谱法(ICP-AES)测定铬质引流剂中Cr2O3、Al2O3、Fe2O3和MgO的分析条件.试样经过氧化钠熔融分解,盐酸酸化,采用内标加入法,利用ICP光谱仪于所推荐的波长处,测量溶液中铬、铝、铁、镁元素对钇内标元素的相对强度,根据标准溶液绘制的校准曲线计算出待测元素氧化物的质量分数.对该方法进行精密度试验,相对标准偏差(RSD,n=8)均小于1.0％,本测试方法简单、快速、精度高,将该方法用于铬质引流剂中Cr2O3、Al2O3、Fe2O3和MgO含量的测定,取得满意效果.     

硫化Mo—K—Rh／Al2O3表面物种的XPS研究

假定单一物种的ＸＰＳ峰形为高斯形，对钼，硫和铑峰进行理论拟合，计算各状态物种表面原子浓度，它们的存在形式各为ＭｏＳ２，富硫环境的ＭｏＳ２＋ｘ，未完全硫化还原的Ｍｏ＾６＋和Ｍｏ＾５＋，Ｓ＾６＋，单质Ｓ＾０或Ｓｎ，Ｓ＾２－和富硫环境中的硫钼结构成（Ｓ－Ｓ）＾２－硫链和Ｒｈ＾ｎ＋（ｎ＝３，２，１，０）。分析发现，催化剂加铑使钼易被硫化还原，铑钼作用可以稳定Ｒｈ＾ｎ＋的存在。     

Luminescence and absorption of Tb3+in mo·Al2O3·B2O3·Tb2O3 glasses

Quantum yields of the green Tb luminescence for 254 nm excitation of glass compositions in the system MO·Al₂O₃· B₂O₃·Tb₂O₃ (M = Mg, Ca, Sr, Ba and Zn) were studied in relation to absorption and excitation spectra. Yields as high as 80% were observed. The Tb 4f-5d absorption maximum ranges from 218 to 232 nm, always at a longer wavelength than the glass matrix absorption. The yield strongly depends on the spectral position of the 4f-5d absorption, due to competing impurity absorption at 254 nm.     

Na2O＊B2O3＊V2O5玻璃的^51V核磁共振研究

本文应用~(51)V核磁共振研究了Na_2O·B_2O_3·V_2O_5玻璃的结构,结果表明: 1)R<0.5+K时,随着R的增加,依次形成NaV_3O_8、NaVO_3和NaVO_3-B结构。 2)R=0.5+K时,全部的V_2O_5转化为NaVO_3和NaVO_3-B结构。 3)R>0.5+K时,由于硼酸盐中非桥氧数的增加,NaVO_3-B结构逐步消失,并推测NaVO_3-B结构中的B原子为四配位结构。     

Na0.15(H3O)0.2CoO2·wH2O的超导电性

最近发现的水合钴氧化物超导体在某些方面具有与高温超导体十分相似的性质.本文报道含有高浓度的水合氢离子的钴氧化物超导体的超导电性磁测量结果.通过对样品的M(H,T)的测量,得到了大致的H～T相图.最后还讨论了系统中可能存在的2D～3D转变.     

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.     

Spectral dispersion of linear optical properties for Sm2O3 doped B2O3–PbO–Al2O3 glasses

Glasses having composition (B₂O₃)₂₅ (PbO)₇₀ (Al₂O₃)₅ (Sm₂O₃)_x ,where x=0, 0.5, 1, 2, 3 and 5 g were prepared using the normal melt quench technique. Spectral reflectance and transmittance at normal incidence of the glass samples are recorded with a spectrophotometer in the spectral range 220–2200 nm. These measured values are introduced into analytical expressions to calculate the real and imaginary parts of the refractive indices. Wemple–DiDomenico single oscillator model and one-term Sellmeier dispersion relations are used to model the real refractive indices. Dispersion parameters such as: single oscillator energy, dispersion energy, lattice oscillating strength, average oscillator wavelength, average oscillator strength and Abbe's number are deduced and compared. Absorption dispersion parameters such as: Fermi energy, optical energy gap for direct and indirect transitions, Urbach energy and steepness parameter are calculated. Effects of doping Sm₂O₃ on these linear optical parameters are investigated and interpreted.