標(biāo)題: Titlebook: RHEED Transmission Mode and Pole Figures; Thin Film and Nanost Gwo-Ching Wang,Toh-Ming Lu Book 2014 Springer Science+Business Media New Yor [打印本頁] 作者: Exaltation 時間: 2025-3-21 16:35
書目名稱RHEED Transmission Mode and Pole Figures影響因子(影響力)
書目名稱RHEED Transmission Mode and Pole Figures影響因子(影響力)學(xué)科排名
書目名稱RHEED Transmission Mode and Pole Figures網(wǎng)絡(luò)公開度
書目名稱RHEED Transmission Mode and Pole Figures網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱RHEED Transmission Mode and Pole Figures被引頻次
書目名稱RHEED Transmission Mode and Pole Figures被引頻次學(xué)科排名
書目名稱RHEED Transmission Mode and Pole Figures年度引用
書目名稱RHEED Transmission Mode and Pole Figures年度引用學(xué)科排名
書目名稱RHEED Transmission Mode and Pole Figures讀者反饋
書目名稱RHEED Transmission Mode and Pole Figures讀者反饋學(xué)科排名
作者: AMITY 時間: 2025-3-21 21:06 作者: 匍匐前進 時間: 2025-3-22 02:21 作者: Anonymous 時間: 2025-3-22 08:14 作者: Cardiac 時間: 2025-3-22 12:28 作者: Cryptic 時間: 2025-3-22 14:54
Gwo-Ching Wang,Toh-Ming Lue correspondence between electrons and spin-orbitals and therefore each electron moves in the average field of the other N-1 electrons /1/. The wave function in this model is the Slater determinant.where the {?.(J)} are a set of N-spin-orbitals and J is the combined space-spin coordinate of electron作者: Fibroid 時間: 2025-3-22 20:25 作者: JOT 時間: 2025-3-22 23:38 作者: corn732 時間: 2025-3-23 03:09 作者: convulsion 時間: 2025-3-23 06:06 作者: Priapism 時間: 2025-3-23 11:53 作者: 反感 時間: 2025-3-23 16:48 作者: manifestation 時間: 2025-3-23 18:34 作者: Tidious 時間: 2025-3-24 01:29 作者: Ambiguous 時間: 2025-3-24 02:49 作者: Dna262 時間: 2025-3-24 08:24
RHEED Reflection Mode,equire a very intense source such as synchrotron radiation. In this chapter, we discuss kinematic treatment of electron scattering and the formulation of angular intensity distribution in both layer-by-layer and multilayer growths. More extensive discussion of RHEED in the transmission mode will be presented in Chaps.?6 and 7.作者: brassy 時間: 2025-3-24 13:16 作者: macabre 時間: 2025-3-24 18:18
Techniques to Control Thin-Film Textures,oretical and Computational Nanotechnology, 729–779, 2005). This opens up endless possibilities for tailoring the desired texture for different applications. In this chapter, we will describe some of the strategies reported recently.作者: 拘留 時間: 2025-3-24 19:51
Introduction,jor applications in molecular beam epitaxy (MBE) growth, is briefly discussed. Then the early work on texture films using RHEED transmission mode and the recent development of RHEED pole figure analysis for textured films are introduced. The importance of the finite inelastic mean free path (IMFP) o作者: ostrish 時間: 2025-3-25 00:09
Crystal Lattices and Reciprocal Lattices,escribed. The commonly used Bravais lattices are summarized. The direction, plane, and interplanar spacing in a real space lattice are defined. The wavevectors, momentum change, Bragg condition, Miller indices, and reciprocal lattice vectors used in wave diffraction are defined. The reason one needs作者: 燈絲 時間: 2025-3-25 03:22 作者: ADAGE 時間: 2025-3-25 10:15 作者: 橫截,橫斷 時間: 2025-3-25 13:08 作者: 埋伏 時間: 2025-3-25 16:22 作者: 粗語 時間: 2025-3-25 23:23
Instrumentation for RHEED Pole Figure,mple manipulator, a step motor, a phosphor screen, and a charge-coupled device camera. Most molecular beam epitaxy (MBE) laboratories with in situ RHEED characterization capability are equipped with this hardware. We discuss what has been learned from past practices on issues such as minimization of作者: 夜晚 時間: 2025-3-26 03:43
Origins of Texture Formation, mechanisms that lead to these different textures are rather complex. They depend on the nature of the substrate (for example, crystalline vs amorphous), substrate temperature, deposition rate, flux energetics, impurities, and deposition geometry. In this chapter, we will provide an overview of some作者: FRAUD 時間: 2025-3-26 05:13 作者: Scleroderma 時間: 2025-3-26 11:42
Applications and Future Directions,alysis. Since electrons interact strongly with matter, RHEED is most suitable for the study of texture when there is a limited amount of sample material. This is the case at the initial stages of the growth of films, where only a small volume of deposits is condensed on the substrate. X-rays interac作者: 套索 時間: 2025-3-26 14:13 作者: CARE 時間: 2025-3-26 17:27 作者: Coordinate 時間: 2025-3-27 00:53 作者: Exterior 時間: 2025-3-27 01:43 作者: 爆米花 時間: 2025-3-27 06:01
the diffraction limitation of processes using optical photons and the technological difficulties connected with x-ray processes, charged particle beams are becoming popular. With them it is possible to write directly on a wafer under computer control, without using a mask. Focused ion beams offer especially g978-1-4612-8247-1978-1-4613-0923-9作者: 兵團 時間: 2025-3-27 12:47
Gwo-Ching Wang,Toh-Ming Lue analyzed the operation of the long magnetic lens. We established the fact that a clear image can only be produced if the particles move close to the field lines. Otherwise, different particles will be focused at different points and the image will be blurred.作者: anatomical 時間: 2025-3-27 17:18
Gwo-Ching Wang,Toh-Ming LuAnalysis) that was coined by Siegbahn for this technique [2]. It is a mistake, however, to take this appellation literally; the applications of the technique transcend chemical analysis, and presentation of even a selected subset of its contributions will require a number of lectures.作者: Culpable 時間: 2025-3-27 21:27
Gwo-Ching Wang,Toh-Ming LuAnalysis) that was coined by Siegbahn for this technique [2]. It is a mistake, however, to take this appellation literally; the applications of the technique transcend chemical analysis, and presentation of even a selected subset of its contributions will require a number of lectures.作者: 脖子 時間: 2025-3-27 22:43
Gwo-Ching Wang,Toh-Ming Luwavelength of the scattered wave does not have to be the same as that for the incident plane wave. If it is the same the wave diffraction is said to be elastic, that is no energy transfer takes place between the incident wave and the diffraction object. If the diffracted wave length is different the作者: mucous-membrane 時間: 2025-3-28 04:10 作者: CIS 時間: 2025-3-28 08:23
Gwo-Ching Wang,Toh-Ming Lupplying the Hohenberg-Kohn-Sham (1,2) local density functional (LDF) formalism, and its recent extension as a local spin density functional (LSDF) formalism (3), to the investigation of various ground state properties of solids despite the usual difficulties of solving the associated one-particle eq作者: 修飾 時間: 2025-3-28 13:41 作者: 把…比做 時間: 2025-3-28 16:14
Applications and Future Directions,m the bulk of the film. The diffraction data obtained from x-rays, on the other hand, inevitably includes information from the bulk of the film (and the substrate) because x-rays have such a large penetration depth. In this sense, RHEED is rather unique for the study of texture at the growth front. 作者: 雕鏤 時間: 2025-3-28 19:58
Book 2014nductors, compound semiconductors, and their characteristics in RHEED pole figures .Provides examples of RHEED measurements of texture and texture evolution, construction of RHEED pole figures, and interpretation of observed pole figures.RHEED Transmission Mode and Pole Figures: Thin Film and Nanost作者: Malfunction 時間: 2025-3-29 01:54
http://image.papertrans.cn/r/image/820132.jpg作者: 細(xì)微差別 時間: 2025-3-29 06:45
https://doi.org/10.1007/978-1-4614-9287-0Crystal Growth; Crystal Lattice; Epitaxial Growth; Nanostructures; RHEED; Reciprocal Lattice; Reflection H作者: Expurgate 時間: 2025-3-29 07:46 作者: sorbitol 時間: 2025-3-29 12:55
Gwo-Ching Wang,Toh-Ming LuPresents a new application of RHEED in the transmission mode.Introduces a variety of textures from metals, semiconductors, compound semiconductors, and their characteristics in RHEED pole figures.Prov作者: Perceive 時間: 2025-3-29 19:02
Introduction,jor applications in molecular beam epitaxy (MBE) growth, is briefly discussed. Then the early work on texture films using RHEED transmission mode and the recent development of RHEED pole figure analysis for textured films are introduced. The importance of the finite inelastic mean free path (IMFP) of electrons in RHEED is emphasized.作者: 相符 時間: 2025-3-29 20:35
X-Ray Diffraction,n for x-ray pole figures using a finite size x-ray area detector and the integration steps to construct x-ray pole figures are covered. The chapter serves as a background for RHEED pole figure construction, which will be discussed in Chap. 6.
