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      非晶     
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  amorphous
    Self-Assembly of Quantum Structure of Amorphous ZnO, Nanocrystalline ZnO & Study of Optical Properties
    非晶态、晶态ZnO量子结构组装及光学特性研究
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    Studies on the Preparation of Nano Amorphous and Intermediate Metastable Phase of α-Quartz-Graphite and Their High Pressure Synthesis and Phase Transition
    α-石英—石墨的纳米非晶和中间亚稳相的制备及其高压合成和相变的研究
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    ON SUPERCONDUCTING TRANSITION TEMPERATURE OF AMORPHOUS TRANSITION METALS
    关于非晶态过渡金属的超导转变温度
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    ORIGIN OF MAGNETIC ANISOTROPY IN AMORPHOUS Gd-Co BASED ALLOY FILMS AND IN CRYSTALLINE FeNi FILMS
    Gd-Co系非晶薄膜垂直于膜面的磁各向异性的起源
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    LOW-TEMPERATURE RESISTIVITY ANOMALIES OBSERVED IN SPUTTERED AMORPHOUS Gd—Co ALLOY FILMS
    非晶态Gd—Co膜中观察到低温电阻率反常现象
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  noncrystalline
    Joint transform real-time optical correlator using noncrystalline film of As_2S_3
    使用非晶态As_2S_3膜的接合变换实时光学相关器
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    RADIAL-DISTRIBUTION FUNCTION (RDF) STUDY OF THE NONCRYSTALLINE STRUCTURE OF POLY P-PHENYLENE SULFIDE (PPS)
    聚对次苯基硫醚(PPS)非晶态结构的径向分布函数研究
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    EXAFS, IR AND RAMAN SPECTRA STUDIES ON THE NONCRYSTALLINE COPPER IONIC CONDUCTORS IN P_2O_5-CuI-CuCl SYSTEM
    P_2O_5-CuI-CuCl系统非晶态铜离子导体的EXAFS,IR,Raman光谱研究
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    Computer Program TRDFA for Radical Distribution Function of Noncrystalline Materials
    非晶态物质径向分布函数微型计算机程序TRDFA
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    The Two--Photon Absorption of Tb~(3+) Ion in Noncrystalline TbP_5O_(14)
    TbP_5O_(14)非晶中Tb~(3+)的双光子吸收
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  an amorphous
    THE HEXAGONAL METASTABLE PHASE FORMED IN AN AMORPHOUS Ni-P ALLOY DURING CRYSTALLIZATION
    非晶Ni-P合金晶化过程中生成的六角亚稳相
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    THE HEXAGONAL METASTABLE PHASE FORMED IN AN AMORPHOUS Ni-P ALLOY DURING CRYSTALLIZATION (II) TWIN GROWTH RELATIONSHIP
    非晶Ni-P合金晶化过程中生成的六角亚稳相(Ⅱ) 孪晶生长关系
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    THE SUPERCONDUCTING TRANSITION TEMPERATURE AND COMPOSITION RANG FOR THE FORMATION OF AN AMORPHOUS PHASE IN THE Mo_xGe_(1-x), Mo_xSi_(1-x) FILMS
    Mo_xGe_(1-x),Mo_xSi_(1-x)薄膜的非晶形成成份及超导转变温度
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    THE HEXAGONAL METASTABLE PHASE FORMED IN AN AMORPHOUS Ni-P ALLOY DURING CRYSTALLIZATION (Ⅲ) HEXAGONAL POLYTYPE
    非晶Ni-P合金晶化过程中生成的六角亚稳相(Ⅲ) 六角多型体
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    THE METASTABLE PHASES FORMED IN AN AMORPHOUS Pd_(80)Si_(20) ALLOY DURING CRYSTALLIZATION
    非晶合金Pd_(80)Si_(20)晶化过程中的亚稳相
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  amorphous phase
    THE SUPERCONDUCTING TRANSITION TEMPERATURE AND COMPOSITION RANG FOR THE FORMATION OF AN AMORPHOUS PHASE IN THE Mo_xGe_(1-x), Mo_xSi_(1-x) FILMS
    Mo_xGe_(1-x),Mo_xSi_(1-x)薄膜的非晶形成成份及超导转变温度
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    THEORETICAL STUDY ON THE FORMATION OF AN AMORPHOUS PHASE IN Fe_xCu_(1-x) BINARY ALLOY SYSTEM
    用原子集团的有序-无序相变理论研究Fe_xCu_(1-x)系统的非晶相形成
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    The results show thathigher Nd content is advalltageous to the formation of amorphous phase.
    实验结果表明,Nd含量的增加有利于非晶相的形成。
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    Full amorphous phase is observed in Al_(82)Fe_5Ni_5Ce_8 after milling for 200h. The crystallization activation energy E was estimated by Kissinger schedule and it is of 164.8kJ·mol~(-1). The effect of cerium is improving the interaction between atoms, and then promoting the capacity of amorphous formation.
    球磨200h后,Al_(82)Fe_5Ni_5Ce_8完全非晶化,晶化激活能为Ec=164.8kJ/mol,具有较好的热稳定性:Al_(90-x)Fe_5Ni_5Ce_x(x=0,2,5,7,8,9)合金的非晶态形成能力,随Ce含量的增加逐渐增强。
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    But LBO crystal becomes an amorphous phase in the pressure range of about 25~31 6GPa and this amorphous transition is irreversible.
    而当压力增加到25~31.6GPa时,LBO出现非晶态,这个非晶化相变是不可逆的。
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  amorphous
       Liquid-Phase Hydrogenation of Chloronitrobenzene Over Pt-Sn-B Amorphous Catalyst Supported by Carbon Nanotubes
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       X-ray diffraction and selected area electron diffraction analysis showed that Pt-Sn-B/CNTs had an amorphous alloy structure that can improve catalytic performance.
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       The hydrodechlorination of CNB was mainly affected by the unique structure of CNTs and the nature of the amorphous metals on the surface of CNTs.
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       The relationship between the interaction of CNTs and amorphous metals and the catalytic performance of the catalyst is also discussed.
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       Results showed that the doped element of Cl lowered the temperatures of phase transformation of TiO2 from amorphous to anatase and from anatase to rutile.
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  noncrystalline
       It is found that the dependence of the fluctuation free volume fraction on the mean coordination number Zm, which characterizes the degree of connectivity of the network in noncrystalline materials, exhibits nonmonotonic behavior.
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       It is found that the temperature coefficient of the SAXS intensity (phonon component) for boron oxide changes at the temperature of the transition from a supercooled liquid state to a solid noncrystalline state.
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       Simulation of noncrystalline silicon nanoparticles: A computer experiment
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       The temperatures of the glass transition and the transition from the supercooled liquid state to the noncrystalline solid state are determined from the temperature dependences of the SAXS intensity.
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       Laser irradiation at a wavelength of 1.5 μm (in an external magnetic field) increases the magnetization of the noncrystalline powder.
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  an amorphous
       X-ray diffraction and selected area electron diffraction analysis showed that Pt-Sn-B/CNTs had an amorphous alloy structure that can improve catalytic performance.
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       3C-SiC nanowires covered by an amorphous shell were obtained on a thin film which was first deposited on silicon substrates, and the nanowires are 20-80 nm in diameter and several μm in length, with a growth direction of [200].
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       Fraction 1 composed of large crystalline blocks comprising particles of initial powder; the second fraction is represented by nanocrystalline blocks with the dimensions of not less than 8 nm; and the third fraction is an amorphous phase.
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       It was shown that, upon annealing, a supersaturated solid solution separates into a solution with the equilibrium concentration X, an intermetallic compound Fe7X6, and an amorphous phase (the effect of "inverse melting").
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       At an energy dose of 12 kJ/g, an amorphous phase of non-uniform composition starts to form in both systems.
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  amorphous phase
       Also, the defects and amorphous phase in CNT films increase with increasing acetylene flow rate.
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       Fraction 1 composed of large crystalline blocks comprising particles of initial powder; the second fraction is represented by nanocrystalline blocks with the dimensions of not less than 8 nm; and the third fraction is an amorphous phase.
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       A decrease in the content and sizes (from 102to 25 nm) of initial microcrystals of fraction 1 is accompanied by the formation of X-ray amorphous phase 3.
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       They are first accumulated synchronously with the amorphous phase and then disintegrated with a decrease in their sizes from 8 to 4 nm.
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       At the initial stage of experiment, at the dose up to 15 kJ/g and the degree of amorphization up to 40%, the energy yield of the formation of amorphous phase amounts to 1 ± 0.1 mol/MJ.
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