氧碘化学激光器废气排放污染评价北大核心CSCD

氧碘化学激光器运行过程中会将氯气、碘蒸气等有毒有害物质排入大气,对工作场所空气质量和人员健康存在安全隐患。采用点源扩散的高斯模式,建立了小风条件下氧碘化学激光器废气的扩散模型,结合工作场地人员分布情况,计算得到激光器废气排放后15min内,距地面1.5m高度、距排放点500m范围内废气中有毒成分氯气和碘的质量浓度空间分布。根据质量浓度空间分布情况,选取采样点,以Na_2SO_3溶液作为吸收液对氯气和碘进行了同时采样,并采取离子色谱测量了吸收液中氯离子和碘离子的质量浓度。结果表明:氧碘化学激光器废气排入大气后,氯气质量浓度最高为0.200mg/m^3,碘蒸气质量浓度小于检测方法的检出限0.030mg/m^3,低于国家职业卫生标准规定的最高容许质量浓度限值1mg/m^3。     

聚对苯撑中杂质诱导的磁性缺陷

本工作研究了掺FeCl₃和掺碘聚对苯撑(PPP)样品中与极化子相互转化有关的电子顺磁共振(EPR)谱特性.在掺碘的样品中,我们观测到一种新的实验现象:室温线宽△H_pp(RT)、自旋浓度N_spin对掺碘浓度的特有依赖关系,即随碘浓度N (Ⅰ)的增大,△H_pp首先减小又增大,然后再次减小重又增大.与此对应,自旋浓度首先升高又下降,然后再次升高又下降.然而,在掺FeCl₃的样品中,△H_pp和N_spin没有出现象在掺碘的样品中那种变化现象,而是随掺FeCl₃浓度增大,△H_pp,首先减小而后增大.相对应地,N_spin首先升高而后下降.本文着重探讨了产生上述差别的原因.由于聚合物链上的自旋和掺杂分子相互作用,观测到的g因子数值接近自由基g值,并且基本上不随掺杂种类、温度的变化而变化.     

模拟核素固化体Gd2Zr2-xCexO7(0≤ x≤ 2.0)的物相及化学稳定性研究

为研究钆锆烧绿石固化Pu(Ⅳ)的相变化情况及化学稳定性, 以Gd₂O₃, ZrO₂为原料, Ce(Ⅳ)作为Pu(Ⅳ)的模拟替代物质, 采用冷压热烧结的方法制备出Gd₂Zr_2-xCe_xO₇(0≤ x≤ 2.0)系列样品. 分别在40 °C和70 °C的合成海水中, 对固化体的长期浸出性能进行研究. 借助粉末X射线衍射仪对所制备样品的物相信息进行收集, 利用等离子体质谱仪对固化体的浸出浓度数据进行分析. 研究结果表明: 当x ≤0.08时, 固化体保持为烧绿石相; 当x>0.08时, 固化体转变为具有缺陷的萤石型结构相. 固化体中Gd³⁺, Zr⁴⁺和Ce⁴⁺在合成海水中, 随着浸泡时间的延长浸出浓度逐渐上升, 70 °C下的浸出浓度高于40 °C下的浸出浓度. 在42 d时, 固化体中Gd³⁺的最大浸出浓度在0.032 μg·ml^-1以下, Zr⁴⁺的最大浸出浓度在0.003 μg·ml^-1以下; Ce⁴⁺的最大浸出浓度在0.032 μg·ml^-1以下.     

激发功率、退火温度及Tm3+浓度对Tm3+/Er3+/Yb3+三掺YF3粉末上转换发光性质的影响

用水热法合成了Tm³⁺/Er³⁺/Yb³⁺三掺杂YF₃上转换发光粉末,并对其进行了结构和形貌表征.对上转换发射谱的研究表明,在相对低激发功率下,可以观察到比较明亮的近白色发光,且随着激发功率的增大,上转换发射强度迅速增大并达到饱和状态,继续增大激发功率,出现发光猝灭现象.退火温度对上转换发射强度的影响表明,随着退火温度的升高,Tm³⁺,Er³⁺的所有特征发射峰均相对增强.上转换发射谱随Tm³⁺浓度变化关系表明,在相对低Tm³⁺掺杂浓度下,Tm³⁺-Er³⁺相互作用占优势,Tm³⁺把能量传递给Er³⁺,Er³⁺发射相对增强;在相对高掺杂浓度下,Tm³⁺-Tm³⁺之间交叉弛豫过程占优势,Er³⁺发射相对减弱.从实验结果看出,该粉末的上转换发光非常丰富,从紫外到红外均有发射,是一种潜在的白色上转换发光及三维固体显示材料.     

添加有TiO2纳米颗粒的R11池沸腾换热研究

对添加有TiO2纳米颗粒的制冷剂R11在外径为22.4mm紫铜管外的池沸腾换热特性进行了实验研究.池沸腾饱和温度为35℃和40℃,纳米颗粒悬浮液的浓度为0.01g/l和0.05g/l.对铜管圆周上、下、前、后四个部位的局部换热情况进行了测量和可视化观察以及相应的粗糙度检测分析.结果发现,纳米颗粒的添加基本使管上部粗糙度降低,传热弱化,而使下部粗糙度增加,传热强化.就整体换热而言,40℃的强化换热效果好于30℃,0.01g/l的强化换热效果好于0.05g/l.     

微弧等离子喷涂碳纳米管/纳米Al2O3-TiO2复合涂层的吸波性能研究

将碳纳米管与纳米Al₂O₃-TiO₂陶瓷粉末超声共混制备了碳纳米管/纳米Al₂O₃-TiO₂复合粉末,测试了复合粉末在2—18GHz波段的电磁参数.研究表明：随着碳纳米管质量分数的增加,碳纳米管/纳米Al₂O₃-TiO₂复合粉末的复介电常数和损耗角不断增大.当碳纳米管质量分数和厚度增加时,复合粉末对电磁波的反射率峰值先增加后减小,而谐振频率不断向低频移动.采用微弧等离子喷涂制备了7wt%碳纳米管/纳米Al₂O₃-TiO₂复合吸波涂层,当厚度为1.5mm时,涂层最小反射率为-24.0dB,当厚度为2.0mm时,涂层小于-10dB的频带宽为3.60GHz,当温度为500℃高温时,1.0mm厚的涂层最小高温反射率为-12.2dB,小于-10dB频带宽为2.0GHz.复合涂层的实际厚度D与理论厚度d呈线关系：d=0.898D+0.515. 关键词： 等离子喷涂 碳纳米管 2O₃-TiO₂')" href="#">纳米Al₂O₃-TiO₂ 吸波性能     

Yb~(3+)/Tm~(3+)共掺杂Sb_2O_4荧光粉的制备及上转换发光性质研究

高温固相法制备了Yb3+/Tm3+共掺的Sb2O4发光粉体,研究了其上转换发光性质。在980nm半导体激光器的激发下,样品发射较强的近红外(800nm)和较弱的蓝色(480nm)及红色(680nm)上转换发光。粉末样品中稀土Yb3+及Tm3+浓度对上转换发光性质具有显著的影响,随着Yb3+或Tm3+浓度的增加,上转换发光增强;Tm3+掺杂浓度达0.8%时其上转换发光强度达到最大,之后上转换发光随Tm3+浓度的增加而减弱,这是由于浓度猝灭引起的。探讨了粉末样品的上转换发光机理,在980nm激发下Tm3+的蓝光和近红外上转换发光均属于二光子的上转换发光过程。     

YZr2OZr3:Er3+纳米晶anti-Stokes发光性质的研究

采用均相沉积法制备了不同Er³⁺离子浓度掺杂的Y₂O₃纳米晶, 应用XRD，SEM和PL光谱对该体系材料进行了表征.在Y₂O₃:Er³⁺纳米材料体系中, 观察和研究了Stokes及anti-Stokes PL谱强度与Er³⁺离子摩尔浓度变化的关系, 当Er³⁺离子浓度为2.0mol%时, anti-Stokes PL强度最强.粉末X 关键词： 氧化钇纳米晶 anti-Stokes PL 双光子吸收     

强磁场对金属离子掺杂CaTiO$lt;sub$gt;3$lt;/sub$gt;结构和光学性能的影响

研究了800 ℃条件下不同制备磁场强度(最高12 T)对CaTiO₃ 及其浸渍掺杂样品在结构和光学性能方面的影响. 研究表明：样品吸光性能随浸渍掺杂的离子浓度的增大而提升,且发生红移现象;相同掺杂浓度下,磁场下制备样品的吸光性能均较非磁场下制备的样品有所提高,但不同磁场强度下所制备样品的吸光曲线彼此差异不大;此外,磁制备纯CaTiO₃晶体粉末的X-射线衍射曲线峰左移,紫外-可见漫反射光谱吸收截止波长增长,这表明强磁场可使CaTiO₃晶面间距和晶格常数增大、禁带宽度减小. 关键词： 3')" href="#">CaTiO₃ 强磁场 掺杂     

金属有机物化学气相沉积生长GaN薄膜的室温热电特性研究

采用金属有机物化学气相沉积技术生长了不同掺杂浓度的GaN薄膜, 并且通过霍尔效应测试和塞贝克效应测试, 表征了室温下GaN薄膜的载流子浓度、迁移率和塞贝克系数. 在实验测试的基础上, 计算了GaN薄膜的热电功率因子, 并且结合理论热导率确定了室温条件下GaN薄膜的热电优值(ZT). 研究结果表明: GaN薄膜的迁移率随着载流子浓度的增加而减小, 电导率随着载流子浓度的增加而增加; GaN 薄膜材料的塞贝克系数随载流子浓度的增加而降低, 其数量级在100–500 μV/K范围内; GaN薄膜材料在载流子浓度为1.60×10¹⁸ cm^-3时, 热电功率因子出现极大值4.72×10^-4 W/mK²; 由于Si杂质浓度的增加, 增强了GaN薄膜中的声子散射, 使得GaN薄膜的热导率随着载流子浓度的增加而降低. GaN薄膜的载流子浓度为1.60×10¹⁸ cm^-3时, 室温ZT达到极大值0.0025.     

Dependence of the magnetic and magnetoelastic properties of cobalt ferrite on processing parameters

The dependence of the magnetic and magnetoelastic properties of highly magnetostrictive cobalt ferrite on processing parameters has been investigated. The cobalt ferrite samples used in this study were prepared via conventional ceramic processing methods. The processing parameters of interest were sintering temperature, holding time at the sintering temperature and powder compaction pressure. It was observed that the crystal structure, composition and saturation magnetization of the samples studied did not vary with changes in processing parameters but coercive field decreased with increasing sintering temperature. The amplitude of peak to peak magnetostriction was dependent on the holding time and powder compaction pressure. The strain derivative on the other hand was found to depend on powder compaction pressure at any given sintering temperature or holding time. The results show how the magnetoelastic properties of cobalt ferrite can be varied by changing the processing parameters.     

Dynamic compression of titanium mononickelide

In this work, the behavior of powdered titanium mononickelide in static and shock compression and subsequent heating of the molds was studied using the methods of x-ray and dilatometric analysis. It was shown that during static compression, in distinction from shock compression, the phase transition B2 B19 takes place to a significant degree in the powder. At the same time, shock compression causes significantly more lattice defects in comparison with static compression, which the process of subsequent sintering activates. During the sintering of the pressings produced by static compression, the reverse transformation takes place in them accompanied by the effect of shape memory and causing the distension of the molds, which complicates the production of high-density sintered material.Translated from Izvestiya Vysshikh Uchebenykh Zavedenii, Fizika, No. 9, pp. 35–39, September, 1987.     

Synthesis and characterization of La0.9Sr0.1Ga0.8Mg0.2O3-δ electrolyte for intermediate temperature solid oxide fuel cells (ITSOFC)

Experimental investigations on new materials for application as electrolyte in electrolyte supported planar Intermediate Temperature Solid Oxide Fuel Cells (ITSOFC) operating below 800 °C is in progress at our laboratory. Sr and Mg doped Lanthanum gallate (LSGM) powder was prepared by glycine — nitrate combustion method. The prepared LSGM powder is relatively finer than that prepared through other techniques such as solid-state reaction. The measurements comprising XRD, particle size, density, TGA/DTA were made. Thin sections of circular pellets were fabricated and annealed at different temperatures ranging between 1000 and 1300 °C. The sintering behaviour of LSGM was investigated to obtain information on the densification factor, relative percentage shrinkage/expansion in volume, while annealing and the resulting apparent porosity values. Bismuth oxide is found to be an effective sintering aid in general. So the effect of bismuth oxide addition on LSGM was investigated through sintering studies, XRD, TGA/DTA, SEM and conductivity measurements. The results obtained on LSGM with and without bismuth oxide addition are discussed with respect to the requirement of an electrolyte for ITSOFC applications. Paper presented at the 2nd International Conference on Ionic Devices, Anna University, Chennai, India, Nov. 28–30, 2003.     

Selective laser sintering of amorphous metal powder

For the first time, selective sintering of amorphous PtCuNiP powder with a pulsed Nd:YAG laser has been studied. Upon pulsed interaction, the grains melt only superficially to build necks between the grains. Depending on the laser parameters, the sintered material can be crystallized or retained amorphous. By contrast with crystalline powder, laser sintering of amorphous powder is achieved at substantially lower pulse energies due to its low melting point. The obtained results are compared with previous results from selective laser sintering of titanium powder. PACS 61.43.Dq; 81.20.Ev, 81.05.Rm     

X-ray diffraction studies on crystallite size evolution of CoFe2O4 nanoparticles prepared using mechanical alloying and sintering

Nanosized cobalt ferrite spinel particles have been prepared by using mechanically alloyed nanoparticles. The effects of various preparation parameters on the crystallite size of cobalt ferrite which includes milling time; ball-to powder weight ratio (BPR) and sintering temperature, were studied using X-ray diffractometer (XRD). Scherrer's equation was used to study the crystallite size evolution of the as-prepared materials. The results of the as-milled sample revealed that both milling time and BPR plays a role in determining the crystallite size of the milled powder. However, where sintering is involved, the sintering temperature results in grain growth, and thus plays a dominant role in determining the final crystallite size of the samples sintered at higher temperature (above 900 °C). From the vibrating-sample magnetometer (VSM) measurement it was observed that the coercivity of the as-milled samples without sintering is almost negligible, which is a type characteristic of superparamagnetic material. However, for the sintered samples, the saturation increases while coercivity decreases with increases sintering temperature.     

Preparation and characterization of flaky FeSiAl composite magnetic powder core coated with MnZn ferrite

The flattening of FeSiAl soft magnetic powder was achieved by ball milling process, and MnZn/FeSiAl composite magnetic powder core was prepared by press molding. The effect of different coating amount of MnZn ferrite on the soft magnetic properties of FeSiAl was studied. At the same time, the optimal stress-relieving annealing temperature of the composite magnetic powder core is revealed. The results showed that the addition of MnZn ferrite affected the magnetic properties such as saturation magnetization (Ms), initial permeability (μi) and power loss (Pcm) of FeSiAl soft magnetic. With the increase of MnZn ferrite addition content, the saturation magnetization of composites decreased gradually, and the magnetic permeability increased first and then decreased, and the loss decreased first and then increased. When the addition content of MnZn ferrite was 5%, the permeability reached the maximum, which was 28.1% higher than that of the pure FeSiAl magnetic powder core under the same conditions. At the same time, the loss was the lowest, which was 13.3% lower than the pure FeSiAl powder core under the same conditions. When the annealing temperature is around 650 °C, the magnetic powder core has the largest magnetic permeability and the lowest loss.     

Study of the sintering behaviour of MgB2 superconductor during hot-pressing

The densification behaviour of MgB₂ was studied when commercial powder was hot-pressed in the temperature range 1070–1190 °C. The mechanisms active during sintering were investigated by continuously recording the shrinkage vs. time and elaborating the data on the basis of Kingery’s model for liquid phase sintering. XRD and SEM analysis on final dense bodies were used to evaluate secondary phases formation during sintering and the effect of magnesium sublimation. AC magnetic susceptibility measurements were also performed to correlate the microstructural and morphological modifications induced by hot-pressing and the superconducting properties.     

聚丙烯酸水溶液及α-A12O3悬浮液的流变性研究

研究了pH、聚丙烯酸（PAA）浓度和分子量对PAA水溶液的粘度的影响,发现溶液的流变行为与溶液中PAA高分子链的离子化程度和构型密切相关,高分子链刚性程度的增加和链的伸展使溶液在pH为7－9时的粘度最大;研究了在PAA溶液中引入陶瓷粉体后悬浮液的粘度变化,发现当陶瓷粉体和PAA的量达到一定比值时悬浮液体系的粘度达到最小值,同时发现陶瓷粉体的粒径大小与这一粘度最小值和悬浮液流变特性也有关。     

Rapid Consolidation by Spark Sintering of Rapidly Solidified 7075 Aluminum Alloy Powder

Compacts of 7075 aluminum have been produced from rapidly solidified powders by optimizing spark sintering parameters, such as pulse discharge time, fixed maximum temperature, holding time at this temperature, and method of cooling to room temperature after the sintering. High-grade compacts can be obtained by a short process (40-50 s) consisting of heating to 773 or 873 K at a heating rate of 9.6 K/s and holding this temperature for 10 s. The rapidly cooled compacts show the same supersaturated state at room temperature as the received as-atomized powder. Compacts quenched in water just after spark sintering at 873 K for 1.2 ks show the same age-hardening behavior as solution-heat treated compacts. Compacts that are quenched in water and aged after sintering at 873 K for 1.2 ks show the same elongation and flow stress as compacts aged after solution heat treatment. Elongation data suggest that compacts produced with longer holding time at a higher temperature and rapid cooling show a large amount of main alloying elements in solid solution and sufficient promotion of sintering.     

Sintering behaviour and microstructures of nanostructured ZnO–ZnS core–shell powder by spark plasma sintering

Densification of nanostructured ZnO–ZnS core–shell powder was carried out by spark plasma sintering to produce a bulk ZnO–ZnS composite. By adjusting the sintering temperature, we could fabricate a bulk ZnO–ZnS composite without destroying the original core–shell structure of the powder. X-ray diffraction and transmission electron microscopy were used to characterize the microstructural properties of the core–shell powder and its sintering behaviour. During spark plasma sintering, phase transition from a sphalerite to a wurtzite structure was observed in the ZnS shell and the crystallographic orientation of the ZnS shell was affected by the ZnO core.