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1.
In situ optical reflectivity measurements are employed to monitor the GaN epilayer growth process above a low-temperature GaN buffer layer on a c-plane sapphire substrate by metalorganic chemical vapour deposition. It is found that the lateral growth of the GaN islands and their coalescence are promoted in the initial growth stage if optimized nitridation time and temperature are selected when the substrate is pre-exposed to ammonia. As confirmed by atomic force microscopy observations, the quality of the GaN epilayers is closely dependent on the surface morphology of the nitridated buffer layer, especially grain size and nucleation density.  相似文献   

2.
薄膜外延生长的计算机模拟   总被引:8,自引:0,他引:8       下载免费PDF全文
以Cu膜为例,用Monte-Carlo算法模拟了薄膜生长的随机过程,并提出了更加完善的模型.在合理选择原子间相互作用计算方法的基础上,考虑了原子的吸附、在生长表面的迁移及迁移所引起的近邻原子连带效应、从生长表面的脱附等过程.模拟计算了薄膜的早期成核情况以及表面粗糙度和相对密度.结果表明,随着衬底温度的升高或入射率的降低,沉积在衬底上的原子逐步由离散型分布向聚集状态过渡形成一些岛核,并且逐步由二维岛核向三维岛核过渡.在一定的原子入射率下,存在三个优化温度,成核率最高时的最大成核温度Tn、薄膜的表面粗糙度最低 关键词: Monte-Carlo算法 计算机模拟 薄膜生长  相似文献   

3.
Comparative analysis of Au, Cu, Pt, Ni and Fe nanoclusters growth on amorphous carbon substrate by proposed kinetic model based on rate equations is present. Partial sticking coefficients introduced into the model let to discriminate elementary processes such as adatom adsorption and diffusion on bare substrate and on top of islands, nucleation and mobility of islands and its coalescence, 2-d and 3-d island growth modes. The quantitative fittings of experimental time dependencies of surface coverage, clusters density, cluster size are performed by solving model equations. From the best fittings the values of phenomenological coefficients defining elementary processes are found for different materials. Comparative analysis of those coefficients let to discover mechanisms of nanoclusters formation and growth of different materials. It is shown that clusterization for Cu and Au is more favorable than for Pt and Ni. Diffusivity for Pt and Ni on amorphous carbon (a-C) substrate is significantly less than for Au and Cu. In opposite, diffusivity on the top of islands for Ni and Pt is significantly higher than for Au and Cu. The mobility of islands for Au and Cu is much higher than for Ni and Pt. The fitting of experimental curves of Fe deposition on a-C at different temperatures showed that temperature mainly influences sticking process but not diffusion.  相似文献   

4.
衬底表面覆盖对薄膜成核和生长的影响   总被引:3,自引:0,他引:3       下载免费PDF全文
邵庆益  方容川  廖源  韩祀瑾 《物理学报》1999,48(8):1509-1513
在薄膜生长的成核阶段,稳定聚集体将逐渐覆盖衬底表面.同时,薄膜的生长将发生在被覆盖的衬底部分,而成核则发生在未被覆盖的部分.本文研究了衬底表面被覆盖的程度对薄膜成核和生长的影响,对广泛应用的薄膜理论,给出一些修正公式.结果表明,成核速率正比于衬底表面未被覆盖面积的平方.而薄膜理论认为成核速率是时间常量,似显得粗糙. 关键词:  相似文献   

5.
动力学晶格蒙特卡洛方法模拟Cu薄膜生长   总被引:3,自引:1,他引:2  
利用动力学晶格蒙特卡洛方法模拟了Cu薄膜在Cu(100)面上的三维生长过程。模型中考虑了四个动力学过程:原子沉积、增原子迁移、双原子迁移和台阶边缘原子迁移,各动力学过程发生的概率由多体势函数确定。讨论了基底温度、沉积速率及原子覆盖率对Cu原子迁移、成核和表面岛生长等微观生长机制的影响;获得了Cu薄膜的表面形貌图并计算了表面粗糙度。模拟结果表明,随基底温度升高或沉积速率下降,岛的平均尺寸增大,数目减少,形状更加规则。低温时,Cu薄膜表现为分形的离散生长,高温时,Cu原子迁移能力增强形成密集的岛。Cu薄膜表面粗糙度随着基底温度的升高而迅速减小;当基底温度低于某一临界温度时,表面粗糙度随原子覆盖率或沉积速率的增大而增大;当基底温度超过临界温度时,表面粗糙度随原子覆盖率或沉积速率的变化很小,基本趋于稳定。  相似文献   

6.
利用Monte Carlo方法研究了基底显微结构对薄膜生长的影响. 对不同显微结构基底上薄膜生长的初始阶段岛的形貌和尺寸与薄膜覆盖度和入射粒子沉积速率之间的关系进行了模拟和分析. 模型中考虑了粒子沉积、吸附粒子扩散和蒸发等过程. 结果表明,基底显微结构对薄膜生长具有明显影响. 当沉积温度为300K、沉积速率为0.005ML/s(Monolayer/second,简称ML/s)、覆盖度为0.05ML时,四方基底上薄膜生长呈现凝聚生长. 随着覆盖度增加,岛的尺寸变大,岛的数目减少. 而对于六方基底,当覆盖度从0.05ML变化到0.25ML时,薄膜生长经历了一个从分散生长过渡到分形生长的过程. 无论是四方还是六方基底,随着沉积速率的增加,岛的形貌由少数聚集型岛核分布状态向众多各自独立的离散型岛核分布状态过渡.  相似文献   

7.
《Physica A》2004,331(1-2):189-197
We present a model equation that describes nucleation and growth of hemispherical nanoclusters or islands deposited on a substrate for the small surface coverage case. The model is formulated in terms of a set of rate equations for the island sizes, combined with the time-dependent behavior of supersaturation and island nucleation rate. As an example to demonstrate the usefulness of the model, we study effects of the deposition rate of adatoms on the nanocluster growth. Large-scale computer simulation results show that the broadness of island size distribution is a decreasing function of the deposition rate for small rates, and bimodal distributions are obtained for large rates.  相似文献   

8.
熊飞  潘红星  张辉  杨宇 《物理学报》2011,60(8):88102-088102
在不同的沉积温度下采用离子束溅射技术,在Si基底上生长得到分布密度高、尺寸单模分布的圆顶形Ge量子点.研究发现:随沉积温度的升高Ge量子点的分布密度增大,尺寸减小,当沉积温度升高到750 ℃时,溅射沉积15个单原子层厚的Ge原子层,生长得到高度和底宽分别为14.5和52.7 nm的Ge量子点,其分布密度高达1.68×1010 cm-2;Ge量子点的形貌、尺寸和分布密度随沉积温度的演变规律与热平衡状态下气相凝聚的量子点不同,具有稳定形状特征和尺寸分布的Ge量子点是 关键词: Ge量子点 离子束溅射沉积 表面原子行为 混晶界面  相似文献   

9.
M.O. Jahma  I.T. Koponen 《Surface science》2007,601(23):5628-5634
We study the optimal conditions for nanoisland growth in ion beam assisted deposition (IBAD). This situation occurs when adatom islands remain small enough to prevent the onset of three-dimensional growth, while at the same time preventing ion-induced surface erosion. To this end, we develop a rate equation model of IBAD, which embodies continuous deposition of adatoms and creation of vacancies, recombination of vacancies at adatom island edges, as well as recombination of adatoms at vacancy island edges. These rate equations are solved by numerical simulations based on the particle coalescence method. To determine the optimal growth condition, we find the largest mean size of the vacancy islands leading to their survival. We show that at this onset between the rough and smooth layer-by-layer growth regimes there is a simple exponential relation between the largest size of the vacancy islands and the external control parameters of the growth.  相似文献   

10.
With a scanning tunneling microscope (STM), we study the initial stage of nucleation and growth of Si on Pb monolayer covered Si(111) surfaces. The Pb monolayer can work as a good surfactant for growth of smooth Si thin films on the Si(111) substrate. We have found that nucleation of two-dimensional (2D) Pb-covered Si islands occurs only when the substrate temperature is high enough and the Si deposition coverage is above a certain coverage. At low deposition coverages or low substrate temperatures, deposited Si atoms tend to self-assemble into a certain type of Si atomic wires, which are immobile and stable against annealing to ~ 200 °C. The Si atomic wires always appear as a double bright-line structure with a separation of ~ 9 Å between the two lines. After annealing to ~ 200 °C for a period of time, some sections of Si atomic wires may decompose, meanwhile the existing 2D Pb-covered Si islands grow laterally in size. The self-assembly of Si atomic wires indicate that single Si adatoms are mobile at the Pb-covered Si(111) surface even at room temperature. Further study of this system may reveal the detailed atomic mechanism in surfactant-mediated epitaxy.  相似文献   

11.
量子点的物理与光电性质主要依赖于其尺寸及密度参数,而量子点的密度、高度等参数又控制着原子在衬底上的成核行为。本文采用液滴外延法在GaAs(001)表面生长金属In液滴,研究了In液滴的扩散运动与衬底温度和沉积速率之间的关系,研究发现,随着衬底温度的升高和沉积速率的降低,In液滴尺寸增大密度却降低。通过得到的实验数据,拟合关于In液滴密度与衬底温度和沉积速率的曲线,分析了量子环的生长机制,并根据原子的表面迁移行为,进一步分析其表面原子扩散机理。  相似文献   

12.
The process of copper deposition on a structured Cu(111)-(9 × 9)-Ag surface, which represents a (9 × 9) loop dislocation network, is studied by scanning tunneling microscopy. It is found that, when the substrate temperature is 100 K and the copper coverage is 0.1–0.4 of a monolayer, islands of a size no greater than 50 Å are formed at the Ag/Cu(111) interface. The islands remain stable as the sample is heated to room temperature. The shape and boundaries of the nanoislands follow the initial surface superstructure and are determined by the nonuniformity of the interaction of the upper silver layer with the copper substrate. The mechanism of island formation and the origin of their stability are explained in terms of the atom exchange between the adsorbate and substrate.  相似文献   

13.
In the early stage of thin film preparation from vapor, growth patterns consisting of stable clusters will gradually cover almost the entire substrate surface. During this process, the density of single atoms is zero on growth patterns and the nucleation of clusters will proceed in the substrate parts uncovered by these patterns. The influence of growth pattern coverage on the nucleation of thin films has not been considered wholly in the classical theory of thin films. We will systematically study the influence of growth pattern coverage and give some correction formulas for the widely used classical theory of thin films. It was found that the classical nucleation rate is proportional to the square of the uncovered area. The corrected formulas are of particular importance in the dominant coverage case.  相似文献   

14.
In present study yttrium-stabilized zirconia (YSZ) thin films were deposited on optical quartz (amorphous SiO2), porous Ni-YSZ and crystalline Alloy 600 (Fe-Ni-Cr) substrates using e-beam deposition technique and controlling technological parameters: substrate temperature and electron gun power which influence thin-film deposition mechanism. X-ray diffraction, scanning electron microscopy (SEM), and atomic force microscopy (AFM) were used to investigate how thin-film structure and surface morphology depend on these parameters. It was found that the crystallite size, roughness and growth mechanism of YSZ thin films are influenced by electron gun power. To clarify the experimental results, YSZ thin-film formation as well evolution of surface roughness at its initial growing stages were analyzed. The evolution of surface roughness could be explained by the processes of surface mobility of adatoms and coalescence of islands. The analysis of these experimental results explain that surface roughness dependence on substrate temperature and electron gun power non-monotonous which could result from diffusivity of adatoms and the amount of atomic clusters in the gas stream of evaporated material.  相似文献   

15.
Thin lithium niobate-tantalate (LiNb0.5Ta0.5O3) films are studied at the initial stage of deposition from a thermal plasma. The effect of two deposition parameters (the substrate temperature and the deposition rate) on the film morphology, the film crystallinity, and the density of nuclei growing on a (0001) sapphire substrate are investigated. It is shown that the crystalline structure and roughness of a film are determined, for the most part, in the initial growth stage and therefore depend directly on both parameters. At the optimum temperatures and growth rates for obtaining good characteristics of (0006) texture, crystallinity, and surface roughness of the films, the film nuclei on the substrate have a high density and good epitaxial orientation to it. If the growth conditions are not optimum, the islands are either amorphous or have a low density on the substrate surface. The nucleation activation energy is observed to decrease as the deposition rate increases, which supports the assumption that the species that are active in film deposition are “hot” clusters forming in an oxygen-argon plasma in the immediate vicinity of the substrate.  相似文献   

16.
Formation of monodispersed Co nanoclusters on a single-crystal Si3N4 dielectric film at room temperature is reported. A remarkably narrow size distribution with the average size of approximately 30 Co atoms has been obtained. We have confirmed that the average size of Co nanoclusters is independent of the Co coverage and the cluster areal density linearly proportions to the Co deposition amount even at high coverages. Also, we have found that Co nanoclusters deposited on Si3N4 are thermally stable with respect to cluster aggregation/coalescence. We propose that this novel phenomenon is a quantum size effect, manifested by local energy minima in the electronic shell structure of Co quantum dots.  相似文献   

17.
利用Monte Carlo(MC)方法,模拟研究了六方晶格基底上薄膜生长的初始阶段岛的形貌和岛的尺寸与薄膜覆盖度以及入射粒子沉积速率之间的关系. 结果表明在基底温度为300K时,岛的形貌主要表现为分形生长,随着薄膜覆盖度的增加,岛的分形枝簇变大,岛的数目不断减少. 在同样的温度下,随着入射粒子沉积速率的增大,薄膜表面的形貌逐步由少数聚集型岛核分布状态向众多各自独立的离散型岛核分布状态过渡. 进一步研究得出,薄膜覆盖度和入射粒子沉积速率对粒子扩散能力的影响最终导致岛的形貌发生了改变.  相似文献   

18.
Many experimental results show that surface roughness of thin films can increase, decrease, stay constant or pass through the minimum with the change in substrate temperature, energy of arriving atoms or assisted beam (electrons, photons, ions), depending on material and interval of variation of those parameters. The aim of this paper is to explain and analyze this non-monotonous behavior of surface roughness by proposed kinetic model. The model is based on rate equations and includes processes of surface diffusion of adatoms, nucleation, growth and coalescence of islands in the case of thin films growth in Volmer-Weber mode. It is shown by modeling that non-monotonous dependence of surface roughness on the factors influencing energy of adatoms (e.g. temperature, assisted beam irradiation, accelerating voltage) occurs as a result of interplay between diffusion length of adatoms and size of islands, because both parameters depend on energy of adatoms. Variation of island size and diffusion length results in atomic jumps from islands forming rougher or smoother surface. The functions of surface roughness, island size, island density on diffusion length of adatoms and on other parameters are calculated and analyzed in this work.  相似文献   

19.
张悦  叶超  王响英  杨培芳  郭佳敏  张苏 《中国物理 B》2017,26(9):95206-095206
The initial growth and microstructure feature of Ag films formation were investigated, which were prepared by using the very-high-frequency(VHF)(60 MHz) magnetron sputtering. Because of the moderate energy and very low flux density of ions impinging on the substrate, the evolutions of initial growth for Ag films formation were well controlled by varying the sputtering power. It was found that the initial growth of Ag films followed the island(Volmer—Weber, VW) growth mode, but before the island nucleation, the adsorption of Ag nanoparticles and the formation of Ag clusters dominated the growth. Therefore, the whole initial stages of Ag films formation included the adsorption of nanoparticles, the formation of clusters, the nucleation by the nanoparticles and clusters simultaneously, the islands formation, and the coalescence of islands.  相似文献   

20.
高温下金属薄膜生长初期的模拟研究   总被引:5,自引:0,他引:5       下载免费PDF全文
吴锋民  施建青  吴自勤 《物理学报》2001,50(8):1555-1559
采用实际的生长模型和物理参量,用Monte Carlo方法对高温下金属薄膜的生长过程进行了模拟研究.综合考虑了原子沉积、扩散、成核、生长和扩散原子的再蒸发、原子沿岛周界扩散和岛的合并等众多过程后,模拟得到与实验结果相当一致的薄膜生长形貌及其相应的定量结果.通过动态统计薄膜生长过程中的岛数目及薄膜生长率,得到实验中不易直接获得的高温下薄膜生长的许多细节,如岛数目和薄膜生长率随表面温度、覆盖度变化的详细情况等 关键词: 薄膜 Monte Carlo模拟 成核 岛密度 薄膜生长率  相似文献   

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