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1.
带电液体基底表面银原子的凝聚和扩散行为   总被引:3,自引:1,他引:2       下载免费PDF全文
金进生  夏阿根  叶高翔 《物理学报》2002,51(9):2144-2149
研究了沉积在带电液体基底(硅油)表面的银原子的凝聚以及扩散行为.先采用热阴极电子发射方法使液体基底表面均匀带电,然后用蒸发沉积方法将银原子沉积到带电的液体基底表面.实验发现:被沉积的银原子首先凝聚成直径约为12μm的准圆形团簇,然后由于库仑排斥力作用而相互离散,所有团簇均向基底的四周边缘漂移;基底表面的团簇数密度n随时间t指数衰减,衰减时间常量Of≈11×10-4s-1;两团簇相互离散的相对平均速率V与它们之间的相对距离L在统计意义上成正比,即V=HL,其中沉积刚结束时常量H≈29×10-4s-1,然后随扩散时间t而逐渐趋于零.分析表明:由于带电银原子团簇的扩散运动,使基底表面的电荷重新分布,基底表面的电场随时间逐渐趋向于处处均匀 关键词: 薄膜 扩散 凝聚  相似文献   

2.
银原子在液体基底上的凝聚特性   总被引:5,自引:0,他引:5       下载免费PDF全文
研究了沉积在液体基底表面上的银原子的扩散和凝聚特性.实验结果表明:银原子在液体表面先形成准圆形的团族,然后通过无规扩散而逐渐凝聚成具有分枝状的凝聚体.准圆形团簇的平均半径以及凝聚速率均随沉积速率的变化而变化.还提出了一个凝聚速率概率模型,计算结果与凝聚速率的实验曲线相符合. 关键词:  相似文献   

3.
采用真空蒸镀方法,利用液体衬底在沉积过程中的线性扩散过程,在玻璃表面制备出斜率仅为10-5的楔形金薄膜逾渗系统,并用四引线方法测量了从该薄膜系统中得到的均匀无序金薄膜的导电特性.实验结果表明:和通常的平整薄膜逾渗系统相比,该薄膜系统呈现更为强烈的跳跃电导和隧道效应. 关键词: 带状薄膜 跳跃电导 隧道效应  相似文献   

4.
含杂质无格点基底表面分枝状凝聚体的计算机模拟   总被引:2,自引:0,他引:2       下载免费PDF全文
根据含杂质熔融玻璃表面金原子凝聚的实验规律,在原子团簇具有随机的线扩散步长和刚性 转动角度的特征条件下,建立了含杂质无格点基底表面的各向异性团簇-团簇凝聚模型,对 团簇的无规扩散、刚性转动以及凝聚全过程进行了计算机模拟,系统地研究了基底表面无规 分布的杂质区域对分枝状凝聚体诸多特性的影响,所得结果与实验事实相符合. 关键词: 薄膜生长 Monte Carlo模拟 分形  相似文献   

5.
楔形Al薄膜的物理特性   总被引:6,自引:0,他引:6       下载免费PDF全文
采用真空蒸镀方法,利用液体衬底在沉积过程中的扩散,形成了沉积在玻璃表面的楔形铝薄膜,并研究了它的结构和I-V特性.实验表明,楔形铝薄膜的斜率仅10-6—10-7,具有与一般非平整薄膜不同的I-V特性,其非平整效应不能用普通的非平整薄膜的RRN理论模型来解释. 关键词: 楔形铝薄膜  相似文献   

6.
本工作确定了一种新型的Ga2S3-Sb2S3-Ag2S硫系玻璃体系的玻璃形成区,研究了玻璃的热稳定性和光学性能、稀土离子掺杂玻璃的中红外发光特性以及玻璃的成纤性能,评估了该玻璃在中红外波段的应用潜力.实验结果表明,Ga2S3-Sb2S3-Ag2S体系的玻璃形成区为~10%—30%Ga2S3,~60%—80%Sb2S3和~0—15%Ag2S(均为摩尔分数);该玻璃具有较宽的红外透过范围(~0.8—13.5μm)、较高的线性折射率(~2.564—2.713@10μm)和较大的三阶非线性折射率(~9.7×10-14—15.7×10-14 cm2/W@1.55μm);使用1.32μm激光抽运,稀土离子Dy...  相似文献   

7.
钱昌吉  高国良  李洪  叶高翔 《物理学报》2002,51(9):1960-1964
由于受基底表面无规分布杂质的影响,沉积在熔融玻璃基底表面的金原子凝聚形成了具有特殊结构的分形凝聚体.根据这一实验结果,建立了各向异性的团簇团簇凝聚模型,对此类胶体基底表面的金原子分枝状凝聚体的生长过程进行了计算机模拟,研究了无规分布的杂质区域对凝聚体各种参数的影响,其结果与实验相符合 关键词: 薄膜生长 MonteCarlo模拟 分形  相似文献   

8.
根据含杂质熔融玻璃表面金原子凝聚的实验规律,在原子团簇具有随机的线扩散步长和刚性转动角的特征条件下,建立了含杂质无格点基底表面上改进的杂质限制团簇-团簇(IRCCA)凝聚模型.对团簇的扩散、刚性转动以及凝聚全过程进行了计算机模拟,系统地研究了杂质区域分布情况对分枝状凝聚体诸多特性的影响.结果表明规则分布的杂质对凝聚体生长的影响比随机分布的杂质大,导致杂质规则分布的基底表面上的分枝状凝聚体的数密度更大,分枝状凝聚体的回旋半径,凝聚体平均大小及分形维数更小. 关键词: 薄膜生长 Monte Carlo模拟 分形 杂质  相似文献   

9.
封面说明     
采用气相沉积方法在液相基底表面成功制备了一种具有近似自由支撑的新型铁薄膜系统.该薄膜的生长机制服从所谓的二阶段生长模型:沉积铁原子在液相基底表面首先成核并凝聚成准圆形原子团簇;然后这些原子团簇在液体表面做无规扩散和旋转运动,从而形成分枝状凝聚体(上图),并随着薄膜名义厚度的增加,分枝状凝聚体逐渐相互连接成网状薄膜,  相似文献   

10.
王玲  王河锦  李婷 《物理学报》2013,62(14):146402-146402
对TiO2粉末进行了空气和真空条件下从室温到1200℃的加热原位X射线衍射实验, 得到了空气和真空条件下微米级锐钛矿颗粒转变为金红石的起始温度分别为850℃ 和855℃; 分别修正了空气条件下锐钛矿在(27–850℃)范围和金红石在(900–1200℃) 范围内的晶胞参数和真空条件下锐钛矿在(27–850℃)范围和金红石在(950–1200℃) 范围的晶胞参数, 从而得到了晶胞参数随温度变化的关系, 得到了锐钛矿和金红石在空气中和真空中的热膨胀系数, 并总结了热膨胀系数随温度变化的规律. 室温下锐钛矿在空气条件下的热膨胀系数为 αa=4.55063×10-6/℃, αc=7.7543×10-6/℃, β=16.85836×10-6/℃; 真空下为 αa=4.69429×10-6/℃, αc=9.02850×10-6/℃, β=18.69688×10-6/℃. 室温下, 金红石在空气条件下的热膨胀系数为 αa=6.81243×10-6/℃, αc=8.71644×10-6/℃, β=22.22178×10-6/℃; 真空条件下为 αa=6.05834×10-6/℃, αc= 8.39280×10-6/℃, β=20.52362×10-6/℃. 关键词: 2')" href="#">TiO2 原位X射线衍射 相转变 热膨胀  相似文献   

11.

It has been shown experimentally that the thermal dissolution of silver and gold thin films in silicate glass is accompanied by the formation of a monolayer of silver and gold micro- and nanocrystals, respectively, on the surface of the glass. These processes occur at temperatures well below the melting temperature of the metal. Microcrystals are formed predominantly at the edges of islands of the metal film, where there is a sufficient amount of the material for their growth. Silver and gold nanocrystals are formed in the case when atoms of the metal dissolved in the glass repeatedly emerge on the glass surface. Silver and gold dissolved in the glass exist not only in the form of atoms and ions but also in the form of charged and neutral molecular clusters.

  相似文献   

12.
It is shown that metallic nanowires (5–8 nm in diameter) that form during laser ablation of Ni, Pb, In, and Sn targets embedded in HeII contain extended single-crystal segments, while spherical clusters (about 2 μm in diameter) that form under these conditions have a regular shape and an atomically smooth surface. Such structures are explained by melting of metal ablation products under their coalescence in HeII. The short-term action of a low-intensity beam of electrons with an energy of 200 keV initiates the explosion in metallic spheres preserved in the vacuum chamber of a transmission electron microscope, which is accompanied with the formation of thousands of clusters with a diameter of a few nanometers. This effect is due to metastability of internal mechanical stresses produced upon sharp cooling of molten spheres by liquid helium. A mechanism of condensation of atoms and nanoparticles in quantized vortices of superfluid helium is proposed.  相似文献   

13.
The yield and energy distributions of sodium atoms upon electron-stimulated desorption from sodium layers adsorbed on tungsten coated with a gold film are investigated for the first time as functions of the thickness of the gold film, the concentration of deposited sodium, and the surface temperature. It is found that the energy distributions exhibit two peaks, namely, a narrow peak with a maximum at about 0.15 eV, whose intensity continuously increases with increasing temperature, and a broad peak with a maximum at about 0.35 eV, whose intensity either decreases or remains constant with increasing temperature. It is shown that both peaks arise as a result of the same excitation, which gives rise to different channels of electron-stimulated desorption of sodium atoms. Possible mechanisms of electron-stimulated desorption and the kinetics of destruction of the surface coating are discussed.  相似文献   

14.
A new model has been developed and calculations have been performed for the formation of nanodroplets after action of an ultrashort laser pulse on a thin (10–100 nm) gold film deposited on a glass substrate. The action of a laser results in the melting of the film in the region of a laser spot and in its thermomechanical separation from the substrate. The separated film acquires a dome shape because of a decrease in the temperature in the direction from the center of the laser spot. This theoretical model provides the explanation of the formation of nanodroplets. It has been established that, first, the separation speed of a gold film from glass decreases sharply because the acoustic impedance of gold is much larger than that of glass. Second, nanodroplets are formed owing to the capillary focusing of the substance, which is manifested in the appearance of the drag component directed toward the axis of symmetry of the dome. The surface tension becomes dynamically significant because of the indicated sharp decrease in the separation speed from glass and of the smallness of the diameter of the focal spot (D ~ 1 μm), which is determined by the diffraction limit of optical radiation.  相似文献   

15.
Laser micromachining on 1000 nm-thick gold film using femtosecond laser has been studied. The laser pulses that are used for this study are 400 nm in central wavelength, 150 fs in pulse duration, and the repetition rate is 1 kHz. Plano-concave lens with a focal length of 19 mm focuses the laser beam into a spot of 3 μm (1/e2 diameter). The sample was translated at a linear speed of 400 μm/s during machining. Grooves were cut on gold thin film with laser pulses of various energies. The ablation depths were measured and plotted. There are two ablation regimes. In the first regime, the cutting is very shallow and the edges are free of molten material. While in the second regime, molten material appears and the cutting edges are contaminated. The results suggest that clean and precise microstructuring can be achieved with femtosecond pulsed laser by controlling the pulse energy in the first ablation regime.  相似文献   

16.
A set of molten gold clusters, each with 1157 gold atoms, was studied by molecular dynamics simulations as the clusters underwent freezing at three different temperatures. Most of the clusters attained an icosahedral structure upon freezing, a structure found to be stable to mild annealing. Other structures observed were imperfect truncated decahedral, truncated octahedral and hexagonal close packed structures. The role of kinetics in the process of cluster solidification is discussed. Received 6 November 2000  相似文献   

17.
左学云  李中秋  王伟  孟利军  张凯旺  钟建新 《物理学报》2011,60(6):66103-066103
利用分子动力学模拟方法,研究了单壁碳纳米管与Au电极的高温熔接. 模拟结果表明,用端口吸附了Au团簇的碳纳米管在高温下能很好地与Au电极熔接. 首先将Au团簇放置于碳纳米管开口处进行高温退火,退火温度在1100 K左右,Au团簇部分Au原子进入碳纳米管管内,吸入碳纳米管中的Au原子形成壳层螺旋结构的Au纳米线,管外Au团簇呈无定形结构. 然后将吸附了Au团簇的碳纳米管与Au电极进行熔接,高温退火后,碳纳米管与Au电极表面之间形成了稳固的熔接,熔接最佳温度在800 K左右. 关键词: 碳纳米管 金电极 分子动力学模拟  相似文献   

18.
为了获得相变温度低且热致变色性能优越的光学材料, 室温下在F:SnO2 (FTO)导电玻璃基板表面沉积钨钒金属膜, 再经空气气氛下的热氧化处理, 制备了W掺杂VO2/FTO复合薄膜, 利用X射线光电子能谱、X射线衍射和扫描电镜对薄膜的结构和表面形貌进行了分析. 结果表明: 高温热氧化处理过程中没有生成W, F, V混合氧化物, W以替换V原子的方式掺杂. 与采用相同工艺和条件制备的纯VO2/FTO复合薄膜相比, W掺杂VO2薄膜没有改变晶面取向, 仍具有(110)晶面择优取向, 相变温度下降到35 ℃左右, 热滞回线收窄到4 ℃, 高低温下的近红外光透过率变化量提高到28%. 薄膜的结晶程度明显提高, 表面变得平滑致密, 具有很好的一致性, 对光电薄膜器件的设计开发和工业化生产具有重要意义. 关键词: W掺杂 2')" href="#">VO2 FTO导电玻璃 磁控溅射  相似文献   

19.
Strong surface (metal) enhanced fluorescence (SEF or MEF) is observed from clusters and single E coli bacteria cells labeled with Carbon nanodots (CDs), which were synthesized from date pits. The enhancement factor (EF) for SEF of the cell clusters were close to 50 for both 533 and 633 nm laser excitation wavelength. Those EFs are ratios of emission peak areas from CD labeled cell clusters on gold film to the peak areas of the same batch cell clusters on glass substrate. SEF with 633 nm excitation performed better than SEF with 532 nm excitation, achieving higher fluorescence intensity and much higher contrast. The contrast as high as 66 for cell clusters on gold film is a ratio of fluorescent emission peak area measured at the CD labeled cell clusters to the fluorescent peak area measured at unlabeled cell clusters (autofluorescence) on the same substrate. The contrast with the background (S/N) or the ratio of fluorescent peak area measured at bacteria cells to area measured at bare substrate was as high as 200. This report may pave a way for the broader application of surface enhanced fluorescence and especially metal enhanced fluorescence imaging of CD labeled cells and other biological objects.
Graphical abstract Carbon dots, synthesized from dates, are used for direct staining of E coli cells. Emission fluorescent spectroscopy of those CD labelled cells on gold film and glass, demonstrated enhancement factor about 50 for emission on gold as compared to glass, Excitation at 633 nm appears far superior to excitation at 532 nm in terms of contrast (up to 67) with unlabeled cells /control due to decrease in auto fluorescence of cells. Maximum Signal to noise ratio is 200.
  相似文献   

20.
Reduction of oxidized gold nanoclusters by exposures to foreign gases and irradiation of UV photons has been investigated using X-ray photoelectron spectroscopy. Gold nanoclusters with narrow size distributions protected by alkanethiolate ligands were deposited on a TiO2(1 1 0) surface with dip coating. Oxygen plasma etching was used for removal of alkanethiolate ligands and oxidization of gold clusters. The oxidized gold clusters were exposed to CO, C2H2, C2H4, H2, and hydrogen atoms. Although, C2H4 and H2 did not show any indications of reduction of oxidized gold clusters, CO, C2H2, and hydrogen atoms reduced the oxides on gold cluster surfaces. Among them, hydrogen atoms were most effective for reduction. Irradiation of UV photons around 400 nm could also reduce the oxidized gold clusters. The photochemical reduction mechanism was proposed as follows. The photo-reduction was initiated by electronic excitation of gold clusters and oxygen atoms activated reacted with carbon atoms at the surfaces of gold clusters. Carbon species were likely absorbed in gold clusters or remained at the boundaries between gold clusters when gold clusters agglomerated during oxygen plasma exposures. As the photochemical reduction progressed, carbon atoms segregated to the surfaces of gold clusters.  相似文献   

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