氮气喷射成形FGH4095的组织特征

以氮气为雾化气体采用喷射成形工艺制备了FGH4095高温合金沉积坯, 记录了沉积过程坯体表面温度曲线, 并采用定量金相法、排水法测试了坯体致密度, 观察了坯体晶粒及γ'相的形貌. 结果表明采用氮气作为雾化介质进行喷射成型喷射沉积坯基体致密度可达99%以上, 但也存在着较大的(1—2μm)的气孔, 经热等静压和近等温锻后宏观气孔闭合, 氮以尺寸不超过1 μm的碳氮化物形式存在. 喷射沉积坯以等轴晶组织为主, 坯体内部平均晶粒尺寸约为20—40 μm, 近表面区域晶粒较细, 约为13 μm; 一次γ' 相多数呈尺寸约0.3—0.5 μm不规则块状形貌. 喷射成形坯组织结构的形成与喷射成形过程的降温过程有密切关系.     

Ultrastructure of Gentiana tibetica proembryogenic cells before and after cooling treatments

The influence of increased concentrations of sucrose, 0.4 M sorbitol, DMSO and vitrification solution (PVS2) on the ultrastructure of non-frozen and frozen suspensions of Gentiana tibetica King ex Hook. F.tissue cells was investigated. Embryogenic aggregates were composed of three groups of cells of different size with various types of plastids. The ultrastructural changes resulting from increasing the sucrose concentration in the medium from 3 to 6 percent for 4 weeks and from treatment with 0.4 M sorbitol for 48 h were similar. Observations showed replacement of large vacuoles by numerous small ones, condensation of cytoplasm, accumulation of starch, and fragmentation of endoplasmic reticulum. Treatment with PVS2 led to degradation of starch, coalescence of amyloplasts and to shrinking of nucleoli from the third group of cells when originating from 6 percent sucrose medium. The mitochondria initially had various shapes, but after PVS2 treatment showed only spherical shapes with sparse cristae. After programmed freezing of tissue protected by sorbitol and DMSO, lethal damage was observed: membrane and nuclei degradation, and cell destruction. Reversible changes after freezing were observed in tissue pretreated with vitrification solution: dilation of cell membranes, mitochondria with electron-lucent vessels, aggregation of numerous vesicles, and degradation of starch in amyloplasts. In cells cooled by a vitrification method, cell organelles appeared normal as early as 5 h after thawing, and anomalies were not observed after 48 h of post-thawing culture.     

Effect of grain boundaries on the conductivity of high-purity ZrO2Y2O3 ceramics

Grain boundary conductivities are determined by complex impedance measurements (1–10⁶ Hz) on high-purity ceramics prepared by the alkoxide synthesis and on less pure ceramics obtained from a commercial powder. The grain size was varied systematically in the region 0.36–55 μm. The grain boundary conductivity is strongly influenced by the grain size, impurities and cooling procedure. The grain boundary conductivity increases linearly with the grain size for small grain sizes (0.3 to 2–4 μm) and is constant for larger grain sizes. The calculated specific conductivity of the grain boundary for pure materials is about 100 times smaller than that of the bulk. The grain boundary thickness was estimated to be 5.4 nm. The activation energy of the grain boundary conductivity is 7 kJ mole^?1 higher than of the bulk.     

Variations in Grain Size Analysis with a Time‐of‐Transition Laser Sizer (Galai CIS‐50) using a Gravitational Flow System

This study deals with grain size analysis with a Laser Sizer Galai CIS‐50. This device utilizes the time‐of‐transition method and is equipped with a module for measurements in the range 0.5 to 150 μm along with a gravitational flow system. Experiments were conducted using natural marine sediments. The aim was to determine possible explanations for discrepancies in the measured results that occurred between different operators of the Galai CIS‐50. These discrepancies may be due to differences in the technique of inserting a sub‐sample into the measurement system. Furthermore, the influence of the sample concentration and the flow velocity in the device's liquid flow cell is considered, since these factors can act as potential sources of inaccuracies and errors in the experimental setup. Strong variations in the results occurred, which were mainly due to problems in the detection of particles >20 μm. In the range>20 μm gaps appeared in the registration of the size distribution. An improvement in reproducibility was achieved by using a pipette instead of a beaker for the insertion step. Nevertheless, the standard deviation for mean grain sizes of natural marine sediments obtained with the Galai CIS‐50 is still about 20%.     

Surface structure of alumina ceramics during irradiation by a pulsed electron beam

The structural transformations that occur in the near-surface layer in alumina ceramics during irradiation by a pulsed electron beam generated by a forevacuum plasma electron source are studied. The modification of the surface properties of the ceramics is shown to be caused by the formation of regions consisting of close-packed and identically oriented crystallites within every grain. The crystallites are elongated: their length and width are 0.5–1.5 μm and the transverse size is 0.1–0.2 μm.     

PDC材料烧结过程中钴在金刚石层中的扩散熔渗迁移机制

 讨论了PDC材料烧结过程中钴在金刚石层中的固相扩散、钴液熔渗、两次钴高浓度峰的“波浪”式迁移过程中的运动规律及其作用机制,并根据实验观测的数据进行了有关计算。结果表明：在5.8 GPa、1 300 ℃条件下,钴的扩散系数D≈1.6×10^-7 cm²/s,是一般常压及相同温度条件下钴固相扩散系数（3×10^-10 cm²/s）和相同压力条件下钴的液相扩散系数（5×10^-5 cm²/s）的中间值;对于粒度W≥10 μm的金刚石烧结体系,钴液熔渗作用时间非常短暂,略大于0.5 s,而对于W≤1 μm的超细金刚石烧结体系而言,钴熔渗作用时间为28 s,比粒度W≥10 μm的金刚石烧结要长得多;两次钴高浓度峰的迁移速度分别约为50 μm/s和100 μm/s。     

Abnormal mitochondrial cristae were experimentally generated by high doses of Apis mellifera venom in the rat adrenal cortex

In the present study, Apis mellifera venom (AmV) was tested for its ability to cause ultrastructural changes in mitochondria of rat adrenal cortex in vivo. In order to achieve this goal, different AmV treatments were performed and the effects were quantified on transmission electron micrographs. In a first experimental group, AmV injected for 30 days in low daily doses (700 μg/kg) generated important ultrastructural changes in zona fasciculata. The mitochondrial ultrastructure was not affected, but the diameters of mitochondrial cristae (MC) were reduced (57.066 ± 7.795 nm) as compared to the MC diameters in the corresponding control groups (58.596 ± 6.603 nm, and 58.503 ± 5.708 nm). In adrenal glands collected from rats injected with a single, high dose of AmV (62 mg/kg), many ultrastructural changes were described. Mitochondria with normal, tubular MC (with diameter of 58.711 ± 5.907 nm) were observed in many cells, very close to the values calculated for the corresponding control group (58.639 ± 6.117 nm). However, the striking data reported herein concerned the ability of AmV high doses to promote dramatic alterations in the ultrastructure of these particular mitochondria, similar to those described in certain severe diseases. Thus, several types of abnormal mitochondria were observed, including mitochondria displaying lamellar and/or circular, concentric cristae and mitochondria devoid of cristae. The abnormal circular, concentric MC, with large inner (281.904 ± 158.588 nm) and outer (432.076 ± 230.372 nm) diameters, appeared to be the most stable form of MC in the adrenal cortex after the acute treatment with AmV. Among other ultrastructural aspects, these important changes indicated a high level of cytotoxicity of AmV in adrenocortical cells following in vivo experimental poisoning.     

金属火灾熔痕的显微组织及物相成分的实验研究

利用X-射线衍射(XRD)和3D图像处理软件(Image-pro)研究了四种不同火灾类型金属熔痕的显微组织、平均晶粒度、物相组成及其分布规律。结果表明：金属火灾熔痕主要由立方晶系的Cu₂O和胞、枝状的Cu组成。在四种不同的起火方式下,金属熔痕的显微组织和成分有显著的差别：(1)一次短路的火灾熔痕平均晶粒度为3～5 μm,其Cu₂O含量最低;过载熔痕的平均晶粒度与一次短路的类似,但其Cu₂O含量为30%左右;(2)二次短路熔痕中含有一定数量直径较大的微观空洞,平均晶粒度约为30 μm;其Cu和Cu₂O衍射峰出现展宽和辟裂,烧蚀程度最深;(3)火灾熔痕中粗大的Cu₂O等轴晶衍射峰强度最大,且显微组织中几乎没有微观空洞存在。     

CLAM钢冲击和拉伸性能测试与研究

对中国低活化马氏体钢——CLAM钢的冲击和拉伸性能进行了测试。结果表明:CLAM钢的塑。脆转变温度在-100℃左右,低于国际上其它几种典型的低活化马氏体钢;在室温和600℃时抗拉强度分别为668和334MPa,类似于EUROFER97的性能。约8μm的晶粒尺寸是CLAM钢具有较好冲击和拉伸性能的主要原因之一。The impact and tensile tests were carried out on the China Low Activation Martensitic steels （CLAM）. The results show: the Ductile-Brittle Transition Temperature （DBTY） is about - 100 ℃, which is lower than those of some other RAFMs; The ultimate strength are 668 MPa at room temperature and 334 MPa at 600℃, which are comparable to those of EUROFER97. The finer grain size of about 8 μm was considered as one of reasons for the superior mechanical properties of CLAM.     

气相生长金刚石膜对衬底金刚石性能的影响

 本文以高压合成金刚石为衬底材料，用热解CVD法在衬底金刚石表面生长了金刚石晶体。结果表明，生长金刚石后的衬底金刚石热性能有明显改善。     

3D imaging of a rice pollen grain using transmission X‐ray microscopy

For the first time, the three‐dimensional (3D) ultrastructure of an intact rice pollen cell has been obtained using a full‐field transmission hard X‐ray microscope operated in Zernike phase contrast mode. After reconstruction and segmentation from a series of projection images, complete 3D structural information of a 35 µm rice pollen grain is presented at a resolution of ～100 nm. The reconstruction allows a clear differentiation of various subcellular structures within the rice pollen grain, including aperture, lipid body, mitochondrion, nucleus and vacuole. Furthermore, quantitative information was obtained about the distribution of cytoplasmic organelles and the volume percentage of each kind of organelle. These results demonstrate that transmission X‐ray microscopy can be quite powerful for non‐destructive investigation of 3D structures of whole eukaryotic cells.     

华南沿海末次冰期类黄土沉积的漫反射光谱与激光粒度研究

野外调查发现,华南沿海广泛发育一套黄色粉土沉积。为研究其特征属性及成因,选择具有代表性的3条粉土剖面及1个钻孔采样,使用漫反射光谱（DRS）分析和激光粒度（LPS）分析的方法,率先尝试从沉积物铁矿物的产出形式和沉积物粒度配分特征的角度,综合判定沉积物的沉积环境、搬运营力及成因机制。DRS分析结果表明,在黄色粉土的漫反射光谱一阶导数曲线中,铁矿物的特征峰峰高总体有赤铁矿（565 nm）>针铁矿(505和435 nm）的变化特征,与我国北方风成黄土的漫反射光谱一阶导数曲线形态吻合,均体现的是相对干冷的气候环境;而区内的河、海相沉积物曲线所反映的铁矿物特征峰的峰高变化与上述黄色粉土的变化方向相反,表明样品经历过充分的水化作用并长期处于潮湿的还原环境之中。LPS分析结果表明：各剖面（钻孔）黄色粉土的粒度组成均较为均一,粒组配分模式具显著的双峰式,两个峰值分别为主峰10～50 μm 区段和次峰<5 μm区段,与黄土沉积的粒度配分模式一致,是风成沉积的特征粒组构成;而与区内河、海相沉积物粒组呈单向变化的配分模式有显著差异。结合黄色粉土的年龄介于10～80 ka之间,以及正负地形皆广泛存在的空间分布特征,最终认为该套沉积是形成于末次冰期的风成沉积（本研究称“类黄土”）。     

六种蜂花粉的红外光谱三级鉴别研究

采用傅里叶变换红外光谱(FTIR)结合二阶导数谱和热扰动下的二维相关红外光谱技术对6种不同花粉,即杏花花粉、油菜花粉、茶花花粉、西瓜花粉、荷花花粉和虞美人花粉,进行了快速无损的鉴别。结果表明,在一维红外光谱图上,不同花粉的蛋白质、脂肪和糖类物质的特征吸收峰在相对峰强和峰位上均存在一定的差异,在二阶导数谱上差异很明显。而在二维红外谱图上,由于6种花粉的自动峰及相关峰峰簇的位置和数量不同,其差别体现得更为明显和直观。因此,三级红外宏观指纹图谱法是鉴别不同蜂花粉种类的一种有效和快速检测方法。     

Zr掺杂形式对钨电子发射材料组织性能的影响

采用中频感应加热烧结方法制备了W-1.5%La₂O₃-0.1%Y₂O₃-0.1%ZrO₂和W-1.5%La₂O₃-0.1%Y₂O₃-0.08%ZrH₂电子发射材料,烧结样品的致密度约为95.5%。热电子发射测试结果表明,添加氢化锆的热电子发射材料样品的零场发射电流密度大于添加氧化锆的样品,分析认为是添加的氢化锆在烧结时,发生分解,生成活性的Zr可以捕获钨晶界中的杂质氧,净化晶界,从而提高了电子发射;维氏显微硬度表明添加氢化锆样品的硬度高于添加氧化锆的样品,分析表明是氢化锆的添加有效改善了钨晶粒之间的结合性,提升了钨电子发射材料的硬度。利用SEM,EDS,XRD、金相显微镜等表面分析设备对样品进行了表征,样品结构显示添加氢化锆与添加氧化锆相比,不仅钨晶粒尺寸由13.63 μm降至11.63 μm,而且稀土相尺寸由1.87 μm降至1.66 μm,这种组织结构的变化有利于电子发射。     

强流脉冲电子束诱发纯镍表层纳米结构的形成机制

利用强流脉冲电子束（HCPEB）技术对多晶纯镍进行了表面处理,并采用扫描电镜和透射电镜对强流脉冲电子束诱发的表面及亚表面的微观组织结构进行了分析.实验结果表明,HCPEB辐照后表面熔化,形成了深度约为2 μm的重熔层,快速的凝固使重熔层中形成晶粒尺寸约为80 nm的纳米结构.位于轰击表面下方5—15 μm深度范围内强烈塑性变形引起的位错墙和其内部的亚位错墙结构是该区域的主要结构特征.这些缺陷结构通过互相交割细化晶粒,最终导致尺寸约为10 nm的纳米晶粒的形成. 关键词： 强流脉冲电子束 纳米结构 多晶纯镍 位错墙     

雪粒径高光谱遥感估算模型研究

雪粒径是影响全球/局地能量收支和表征积雪水热状态的重要参数,大面积监测和估算雪粒径的分布及大小对于全球/局地气候变化和水资源管理具有重要意义。目前遥感技术已成为大面积监测和估算雪粒径的重要手段。针对雪粒径的遥感监测与估算,该研究采用辐射传输模型模拟雪面可见光-近红外波段的光谱曲线,经过分析光谱曲线并结合一阶微分和累计差异值选取对雪粒径敏感的波段和积雪指数,建立单变量雪粒径高光谱遥感估算模型,并用地面实测数据进行验证,结果表明,单波长1 030 nm,1 260 nm和归一化差值积雪指数(460和1 030 nm)构建的估算模型预测精度较高,雪粒径估算值与实测值的相关斜率分别为1.37,0.61和0.62 ,R2分别为0.82,0.86和0.93,RMSE分别为55.65,50.83和35.91 μm,可用于雪粒径的估算研究。研究成果为雪粒径的高光谱遥感反演提供科学依据。     

北疆地区不同雪粒径光谱特征观测及反演研究

雪粒径反演是冰冻圈遥感的重要研究内容之一。本研究通过设计不同雪粒径观测方案,在我国北疆地区利用SVC HR-1024野外便携式光谱仪观测了不同雪粒径的光谱特征;同时利用可拍照显微镜测量了雪粒径的大小和形状,并通过DSPP方法计算其等效粒径;最后,基于渐进式积雪辐射传输模型(ART)对反演波段和积雪形状因子进行优化,反演并验证雪粒径。研究表明DSPP方法获取积雪等效粒径是可行的,但由于同层积雪中样本选择存在较大差异,在样本选择方面需要进一步改进;近红外波段还是区分雪粒径的有效波段,在研究区积雪是干雪的条件下,基于ART优化反演波段和积雪形状因子优化方法反演雪粒径是可行的,根据试验获取在该地区雪粒径反演最佳波段为1.20 μm,最佳积雪形状因子b值为3.62。     

Synthesis and microstructure analysis of composite Nd:YAG/YAG transparent ceramics

Transparent Nd：YAG/YAG composite ceramics are synthesized by solid-state reaction method using high- purity Y203, A1203, and Nd203 powders as raw materials. The mixed powder compacts are sintered at 1780 ℃ for 10 h under vacuum and annealed at 1450 ~C for 20 h in air. The Nd：YAG/YAG ceramics exhibit a pore free structure with an average grain size of about 30 μm. The microstructure of the Nd：YAG/YAG composite transparent ceramics is studied and there is no interface between Nd：YAG and YAG ceramics. The Nd ion distribution in one grain is also studied, which shows that there is no segregation of Nd ions as in Nd：YAG crystals.     

Fabrication of large-grain polycrystalline silicon for solar cells

The rapid recrystallization of a-Si films utilizing excimer laser crystallization (ELC) is investigated. The melt duration of liquid silicon (liquid Si) is measured by in-situ time-resolved optical measurements during ELC. The grain size of crystallized poly-Si films are characterized by FE-SEM. The substrate temperature as a function of the longest melt duration of liquid Si for different Si film thicknesses are presented. In-situ timeresolved optical measurements reveal that the longest melt duration of 400-nm-thick a-Si thin films at a substrate temperature of 500 °C is 1714 ns. The diameter of the disk grain as large as 4.7 μm is produced by ELC, which can be applied to solar cells with a high conversion efficiency and reliability.