106 resultados para Ta-Cu composites

em Chinese Academy of Sciences Institutional Repositories Grid Portal


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实验结果表明Ta/NiFe/FeMn/Ta多层膜的交换耦合场Hex要大于Ta/NiFe/Cu /NiFe/FeMn/Ta自旋阀多层膜中的Hex. 为了寻找其原因, 用X射线光电子能谱(XPS)研究了Ta(12 nm)/NiFe(7 nm), Ta(12 nm)/NiFe(7 nm)/Cu(4 nm)和Ta(12 nm)/NiFe(7 nm)/ Cu(3 nm)/NiFe(5 nm) 3种样品, 研究结果表明前两种样品表面无任何来自下层的元素偏聚, 但在第3种样品最上层的NiFe表面上, 探测到从下层偏聚上来的Cu原子. 认为: Cu在NiFe/FeMn层间的存在是Ta/NiFe/Cu/NiFe/FeMn/Ta自旋阀多层膜的Hex低于Ta/NiFe/FeMn/Ta多层膜Hex的一个重要原因.

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Graphite-flake reinforced Cu47Ti34Zr11 Ni-8 bulk metallic glass matrix composite was fabricated by water-cooled copper mould cast. Most of the graphite flakes still keep unreacted and distribute uniformly in the amorphous matrix except that some reactive wetting occurs by the formation of TiC particles around the flakes. It reveals that the presence of graphite flakes does not affect the onset of the glass transition temperature, crystallization reaction and liquidus of the metallic glass. The resulting material shows obvious serrated flow and higher fracture strength under room temperature compressive load, comparing with the monolithic bulk metallic glass (BMG). Three types of interaction between the shear bands and graphite flakes, namely, shear band termination, shear bands branching and new shear bands formation near the graphite flakes can be observed by quasi-static uniaxial compression test and bonded interface technique through Vickers indentation.

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Experimental results show that the exchange coupling field (H-ex) of NiFe/FeMn for Ta/NiFe/FeMn/Ta multilayers is higher than that for spin-valve multilayers Ta/NiFe/Cu/NiFe/FeMn/Ta. In order to find out the reason, the composition and chemical states at the surface of Ta(12 nm)/NiFe(7 nm), Ta(12 nm)/NiFe(7 nm)/Cu(4 nm), and Ta(12 nm)/NiFe(7 nm)/Cu(3 nm)/NiFe(5 nm) were studied using x-ray photoelectron spectroscopy. The results show that no elements from lower layers float out or segregate to the surface in the first and second samples. However, Cu atoms segregate to the surface of Ta(12 nm)/NiFe(7 nm)/Cu(3 nm)/NiFe(5 nm) multilayers, i.e., Cu atoms segregate to the NiFe/FeMn interface for Ta/NiFe/Cu/NiFe/FeMn/Ta multilayers. We believe that the presence of Cu atoms at the interface of NiFe/FeMn is one of the important factors which causes the exchange coupling field (H-ex) of Ta/NiFe/Cu/NiFe/FeMn/Ta to be weaker than that of Ta/NiFe/FeMn/Ta. (C) 2002 American Institute of Physics.

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Zr49Cu46Al5 and Zr48.5Cu46.5Al5 bulk metallic glasses(BMGs) with diameter of 5 mm were prepared through water-cooled copper mold casting. The phase structures of the two alloys were identified by X-ray diffractometry(XRD). The thermal stability was examined by differential scanning calorimetry(DSC). Zr49Cu46Al5 alloy shows a glass transition temperature, T, of about 689 K, an crystallization temperature, T-x, of about 736 K. The Zr48.5Cu46.5Al5 alloy shows no obvious exothermic peak. The microstructure of the as-cast alloys was analyzed by transmission electron microscopy(TEM). The aggregations of CuZr and CuZr2 nanocrystals with grain size of about 20 nm are observed in Zr49Cu46Al5 nanocrystalline composite, while the Zr48.5Cu46.5Al5 alloy containing many CuZr martensite plates is crystallized seriously. Mechanical properties of bulk Zr49Cu46Al5 nanocrystalline composite and Zr48.5Cu46.5Al5 alloy measured by compression tests at room temperature show that the work hardening ability of Zr48.5Cu46.5Al5 alloy is larger than that of Zr48.5Cu46.5Al5 alloy.

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Using a first-principles method, we investigate the structural and electronic properties of grain boundaries (GBs) in polycrystalline CdTe and the effects of copassivation of elements with far distinct electronegativities. Of the two types of GBs studied in this Letter, we find that the Cd core is less harmful to the carrier transport, but is difficult to passivate with impurities such as Cl and Cu, whereas the Te core creates a high defect density below the conduction band minimum, but all these levels can be removed by copassivation of Cl and Cu. Our analysis indicates that for most polycrystalline systems copassivation or multipassivation is required to passivate the GBs.

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The experimental results show that the exchange coupling field H.. of NiFe/FeMn for TalNiFe/FeMn/Ta multilayers is higher than that for the spin valve multilayers Ta/NiFe/Cu/NiFe/FeMn/Ta. The composition and chemical states at the surface of Ta(12nm)/NiFe(7nm), Th(12nm)/NiFe(7nm)/Cu(4nm) and Ta(12nm)/NiFe(7nm)/Cu(3 nm)/NiFe(5 mn) were studied by using x-ray photoelectron spectroscopy. The results show that no element from the underlayers Boats out or segregates to the surface for Th(12 nm)/NiFe(7nm), Ta(12 nm)/NiFe(7nm)/Cu(4 mn). However, Cu atoms segregate to the surface of Ta(12 nm)/NiFe(7nm)/Cu(3nm)/NiFe(5nm) multilayers, i.e. to the NiFe/FeMn interface for Ta/NiFe/Cu/NiFe/FeMn/Ta multilayers. We believe that the presence of Cu atoms at the interface of NiFe/FeMn is one of the important factors which will cause the exchange coupling field H.. of Ta/NiFe/FeMn/Ta multilayers to be higher than that of Ta/NiFe/Cu/NiFe/FeMn/Ta multilayers.

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We report new results on identified (anti) proton and charged pion spectra at large transverse momenta (3 < p(T) < 10 GeV/c) from Cu + Cu collisions at root s(NN) = 200 GeV using the STAR detector at the Relativistic Heavy Ion Collider (RHIC). This study explores the system size dependence of two novel features observed at RHIC with heavy ions: the hadron suppression at high-p(T) and the anomalous baryon to meson enhancement at intermediate transverse momenta. Both phenomena could be attributed to the creation of a new form of QCD matter. The results presented here bridge the system size gap between the available pp and Au + Au data, and allow for a detailed exploration of the onset of the novel features. Comparative analysis of all available 200 GeV data indicates that the system size is a major factor determining both the magnitude of the hadron spectra suppression at large transverse momenta and the relative baryon to meson enhancement.

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Ti40Cu40Ni10Zr10-xScx (x = 0.5 and 1, at%) alloys were prepared by copper mould casting method. Microstructures of the phi 3 mm rod alloys were investigated by XRD and SEM. The results showed that the phi 3 mm rods were glassy matrix with TiCu crystalline phase. Mechanical properties were studied by compressive test. Ti40Cu40Ni10Zr9Sc1 alloy exhibited good compressive strength over 2200 MPa and superior compressive deformation is about 7.9%.

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在峨眉山大火成岩省(ELIP)产出许多岩浆Cu-Ni-PGE岩浆硫化物矿床,如金宝山、杨柳坪、力马河、白马寨,以及大槽-阿布郎当矿化岩体。根据成矿元素组成特征,这些矿床可以区分为多种不同矿化类型,有以铂族元素为主贫铜镍的矿床,如金宝山Pt-Pd矿床;有含较高铂族元素和铜镍的矿床,如杨柳坪Ni-Cu-PGE矿床;也有贫铂族元素富铜镍的矿床,以力马河和白马寨Ni-Cu矿床最为典型。造成峨眉山大火成岩省中Ni-Cu-PGE岩浆硫化物矿床矿化类型变异的原因是什么?它们的母质岩浆性质如何,产生于怎样的熔融程度?既然能形成岩浆硫化物矿床,造成硫化物熔离的原因有哪些,什么因素起到了关键作用?这些矿化类型多样的Ni-Cu-PGE矿床的成矿岩浆有何差异?产生差异的原因是什么?带着这些疑问,通过借鉴国内外Ni-Cu-PGE岩浆硫化物矿床研究的经验,本文以金宝山铂钯矿、力马河镍矿及大槽-阿布郎当岩体的地球化学研究为基础,结合近几年来前人对杨柳坪,白马寨等矿床的系统研究,本文试图解决上述疑问。现在取得的主要认识有: 1) 根据成矿元素组成特征,可以把峨眉山大火成岩省中(ELIP)存在的Ni-Cu-PGE岩浆硫化物矿床分成多种不同的矿化类型,包括PGE矿床(例如金宝山Pt-Pd矿),Ni-Cu-PGE矿床(例如杨柳坪矿床),Ni-Cu矿床(例如力马河和白马寨矿床),以及弱矿化或不含矿的超镁铁质堆晶岩体(例如大槽-阿布郎当岩体)。通过对ELIP中几种类型Cu-Ni-PGE矿床成矿母岩浆的研究发现,它们均具有类似峨眉山苦橄岩的成分特征,表明母岩浆形成于较高程度的地幔部分熔融,并富集Ni和PGE。 2)硫化物熔离的多阶段性是导致矿床类型变异的一个重要因素。早期结晶矿物的分离结晶导致了金宝山母岩浆出现S的饱和,少量的浸染状硫化物被携带进入岩浆通道中发生了沉淀,继续富集PGE,形成了金宝山矿体。杨柳坪的母岩浆先发生了少量早期硫化物熔离丢失,PGE弱亏损的岩浆在后期上升过程中由于强烈的地壳混染,发生了大量硫化物熔离并发生堆积,形成杨柳坪矿体。力马河和白马寨的母岩浆在早期发生了较多的硫化物丢失,PGE强烈亏损的岩浆发生了二次以上的硫化物熔离,形成了力马河和白马寨矿体。 3) R因子(岩浆与熔离硫化物的比例)是决定ELIP中Cu-Ni-PGE矿床矿化类型变异的重要因素。金宝山矿床具有极高的R值(>10000),杨柳坪和朱布矿床具有中等的R值(2000~5000),而力马河矿床近似为在经过R=2000的硫化物熔离之后,残余岩浆再经过R=200的硫化物熔离。 4) 地壳混染程度的差异可能是造成ELIP中Ni-Cu-PGE矿床矿化类型发生变异的关键因素。金宝山矿床的地壳混染程度较低,可能主要是早期橄榄石和铬铁矿的分异结晶导致了岩浆中硫化物出现了饱和。对于大槽-阿布郎当矿化岩体,只是在岩体边缘的局部出现了硫化物熔离,可能是围岩混染造成的。对于杨柳坪Ni-Cu-PGE矿床、力马河和白马寨Ni-Cu矿床,从微量元素蛛网中明显的Nb-Ta负异常,高放射成因187Os丰度的初始Os同位素组成(γOs(t)=100~120),S同位素等反映出显著的地壳混染,因而出现大量硫化物熔离。

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Based on the 'average stress in the matrix' concept of Mori and Tanaka (:Mori, T., Tanaka, K., 1973. Average stress in matrix and average elastic energy of materials with misfitting inclusion. Acta Metall. 21, 571-580) a micromechanical model is presented for the prediction of the elastic fields in coated inclusion composites with imperfect interfaces. The solutions of the effective elastic moduli for this kind of composite are also obtained. In two kinds of composites with coated particulates and fibers, respectively, the interface imperfections are takes to the assumption that the interface displacement discontinues are linearly related to interface tractions like a spring layer of vanishing thickness. The resulting effective shear modulus for each material and the stress fields in the composite are presented under a transverse shear loading situation.

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The stiffness behaviour of injection moulded short glass fibre/impact modifier/polypropylene hybrid composites has been investigated in this work by theoretical predictions and experiments. Predictions from the self-consistent method were found to be in good agreement with test results for the impact modifier/polypropylene blends. By taking into account of the fibre orientation distributions in the skin and core layers, the values of Young's modulus for the skin and core layers were predicted by employing Eshelby's equivalent inclusion method and the average induced strain approach. The prediction of the values of Young's modulus for the whole sample was obtained by applying the simple mixture theory of laminated composites to the predicted results for the skin and core layers. Good correlation between predicted and experimental Young's modulus values were found.

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The strengthening behavior of particle-reinforced metal-matrix composites (MMCp) is primarily attributed to the dislocation strengthening effect and the load-transfer effect. To account for these two effects in a unified way, a new hybrid approach is developed in this paper by incorporating the geometrically necessary dislocation strengthening effect into the incremental micromechanical scheme. By making use of this hybrid approach, the particle-size-dependent inelastic deformation behavior of MMCp is given. Some comparisons with the available experimental results demonstrate that the present approach is satisfactory.

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For metal-matrix composites (MMCs), interfacial debonding between the ductile matrix and the reinforcing hard inclusions is an important failure mode. A fundamental approach to improving the properties of MMCs is to optimize their microstructure to achieve maximum strength and toughness. Here, we investigate the flow stress of a MMC with a nanoscale microstructure similar to that of bone. Such a 'biomorphous' MMC would be made of staggered hard and slender nanoparticles embedded in a ductile matrix. We show that the large aspect ratio and the nanometer size of inclusions in the biomorphous MMC lead to significantly improved properties with increased tolerance of interfacial damage. In this case, the partially debonded inclusions continue to carry mechanical load transferred via longitudinal shearing of the matrix material between neighboring inclusions. The larger the inclusion aspect ratio, the larger is the flow stress and work hardening rate for the composite. Increasing the volume concentration of inclusion also makes the biomorphous MMC more tolerant of interfacial damage.

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Aimed at brittle composites reinforced by randomly distributed short-fibers with a relatively large aspect ratio, stiffness modulus and strength, a mesoscopic material model was proposed. Based on the statistical description, damage mechanisms, damage-induced anisotropy, damage rate effect and stress redistribution, the constitutive relation were derived. By taking glass fiber reinforced polypropylene polymers as an example, the effect of initial orientation distribution of fibers, damage-induced anisotropy, and damage-rate effect on macro-behaviors of composites were quantitatively analyzed. The theoretical predictions compared favorably with the experimental results.

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A three-phase piezoelectric cylinder model is proposed and an exact solution is obtained for the model under a farfield antiplane mechanical load and a far-field inplane electrical load. The three-phase model can serve as a fiber/interphase layer/matrix model, in terms of which a lot of interesting mechanical and electrical coupling phenomena induced by the interphase layer are revealed. It is found that much more serious stress and electrical field concentrations occur in the model with the interphase layer than those without any interphase layer. The three-phase model can also serve as a fiber/matrix/composite model, in terms of which a generalized self-consistent approach is developed for predicting the effective electroelastic moduli of piezoelectric composites. Numerical examples are given and discussed in detail.