(C.Boulmer-Leborgne
,
J.Hermann and B.Dubreuil GREMI
,
Orleans University. CNRS
,
France)I. Ursu
,
M.Dinescu
,
N
,
Chitica and I.N.Mihailescu (Institute of Atomic Physics
,
Bucharest
,
Romania)(International Center for Theoretical Physics.Trieste
,
Italy)
材料科学技术(英文)
We have investigated the role of the ambient gas nature and pressure in the structure and appearance of the laser treated zone. and the influence of the total duration and temporal shape of laser pulse with the laser tight being λ= 10.6μm wavelength incident upon a metallic surface at intermediate taser intensities of 107-108 W / cm2. A plasma is accompanied by the action of the laser pulse, It acts as an active moderator among laser beam and target thus determining the final status of the contact surface
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Applied Physics Letters
A hydrothermal approach was developed for the synthesis of N-doped graphene quantum dots (N-GQDs) by cutting N-doped graphene. The N-GQDs obtained have a N/C atomic ratio of ca. 5.6% and diameter of 1-7 nm. The photoluminescence (PL) properties of the N-GQDs were investigated. It was found that the N-GQDs possess bright blue PL and excellent upconversion PL properties. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4750065]
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oxygen reduction
Journal of Spacecraft and Rockets
An amorphous silicon carbonitride (Si(1-x-y)C(x)N(y), x = 0.43, y = 0.31) coating was deposited on polyimide substrate using the magnetron-sputtering method. Exposure tests of the coated polyimide in atomic oxygen beam and vacuum ultraviolet radiation were performed in a ground-based simulator. Erosion kinetics measurements indicated that the erosion yield of the Si(0.26)C(0.43)N(0.31) coating was about 1.5 x and 1.8 x 10(-26) cm(3) /a tom during exposure in single atomic oxygen beam, simultaneous atomic oxygen beam, and vacuum ultraviolet radiation, respectively. These values were 2 orders of magnitude lower than that of bare polyimide substrate. Scanning electron and atomic force microscopy, X-ray photoelectron spectrometer, and Fourier transformed infrared spectroscopy investigation indicated that during exposures, an oxide-rich layer composed of SiO(2) and minor Si-C-O formed on the surface of the Si(0.26)C(0.43)N(0.31) coating, which was the main reason for the excellent resistance to the attacks of atomic oxygen. Moreover, vacuum ultraviolet radiation could promote the breakage of chemical bonds with low binding energy, such as C-N, C = N, and C-C, and enhance atomic oxygen erosion rate slightly.
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atomic oxygen;films;radiation;polymers;beam;sicn
Journal of Chemical Physics
Based on Mei's embedded atom model [Mei , Phys. Rev. B 43, 4653 (1991)] molecular dynamics simulations have been performed to investigate the rapidly cooling processes of Cu. The atomic transport property, namely the self-diffusion coefficient, is computed in the liquid state, and the results near the melting point of Cu are in good agreement with experimental data and other computational values. The atom diffusion movements during the long period of relaxation have been also studied around the solidification temperature T-c. To describe the complex microstructural evolutions during the rapidly cooling processes and the long relaxation processes, the pair correlation function and the pair analysis technique are used. It is demonstrated that the crystallization of amorphous Cu is caused by the atomic diffusion. (C) 2004 American Institute of Physics.
关键词:
transition-metals;computer-simulation;supercooled-liquid;model;fcc;potentials;diffusion
葛庆麟
,
施天生
,
陈廷国
,
陈源
,
吴自良
金属学报
四种不同Ti浓度的Fe-Ti合金,加氮到N/Ti>1之后,发现有两个内耗峰,并且随氮浓度之增加而同时升高。20℃处的峰是氮的Snoek峰,160℃附近的是s-i峰。s-i峰的峰高和Ti浓度成线性关系,表明起峰的反应只涉及孤立的Ti原子,与Ti-Ti原子对或杂质原子团都无关系。 提出了产生s-i峰的二种缺陷中心——Ti-N对缺陷和N-Ti-N仨缺陷——的模型(图7)。氮占Ti位就构成对缺陷,其中的Ti,N原子亲和力很强,只要合金中尚存有自由Ti原子,就不可能存有自由氮原子,因此N/Ti≤1以下,不会出现Snoek峰或s-i峰。N/Ti>1之后,多余氮原子要在对缺陷的OⅡ位和T_3位之间以约1:10的比例进行分配,直到绝大部分的对缺陷转化为仨缺陷。N/Ti(?)2以后,几乎所有的多余氮都进入了仨缺陷的OⅡ位,此时s-i峰的弛豫强度突然增加10倍。 淬火时冻结在α-Fe基体中的过饱和氮、要扩散到OⅡ位(扩散距离~10(?)),以期达到室温下的再分配,因此引起Snoek峰室温下的迅速衰减。s-i峰的形状,只取决于多余氮的浓度,与淬火温度、冷却速度无关。
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