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Interfaces grain boundaries

Extended defects range from well characterized dislocations to grain boundaries, interfaces, stacking faults, etch pits, D-defects, misfit dislocations (common in epitaxial growth), blisters induced by H or He implantation etc. Microscopic studies of such defects are very difficult, and crystal growers use years of experience and trial-and-error teclmiques to avoid or control them. Some extended defects can change in unpredictable ways upon heat treatments. Others become gettering centres for transition metals, a phenomenon which can be desirable or not, but is always difficult to control. Extended defects are sometimes cleverly used. For example, the smart-cut process relies on the controlled implantation of H followed by heat treatments to create blisters. This allows a thin layer of clean material to be lifted from a bulk wafer [261. [Pg.2885]

The performance characteristics of ceramic sensors are defined by one or more of the foUowing material properties bulk, grain boundary, interface, or surface. Sensor response arises from the nonelectrical input because the environmental variable effects charge generation and transport in the sensor material. [Pg.345]

Table 1 Concentration of major solute elements at grain boundary, interface, and matrix in the Si3N4/5052 Al composite... Table 1 Concentration of major solute elements at grain boundary, interface, and matrix in the Si3N4/5052 Al composite...
The grain boundary interfaces are clean and essentially flat on the atomic scale, but contain large misorientations, as shown in Figure 12 (48). Grain B is [110] 2212 phase, and grain C is strontium-copper oxide. [Pg.582]

Figure 17 (a) Grain boundary interface with amorphous region at the triple point, (b) EDX from the area x, showing mostly copper (oxide). [Pg.595]

The surface of a solid sample interacts with its environment and can be changed, for instance by oxidation or due to corrosion, but surface changes can occur due to ion implantation, deposition of thick or thin films or epitaxially grown layers.91 There has been a tremendous growth in the application of surface analytical methods in the last decades. Powerful surface analysis procedures are required for the characterization of surface changes, of contamination of sample surfaces, characterization of layers and layered systems, grain boundaries, interfaces and diffusion processes, but also for process control and optimization of several film preparation procedures. [Pg.277]

Figure 10-15. Interaction potential between the (moving) grain boundary (interface) and solute species i, and its spatial distribution c, at t = 0. Figure 10-15. Interaction potential between the (moving) grain boundary (interface) and solute species i, and its spatial distribution c, at t = 0.
Based on conceptions of work [105] the specific dielectric relaxation in PPX with M nanoparticles is supposed to be connected with reorientation of dipoles in polymer environment of M nanoparticles that accompanies the electron transfer between M nanoparticles of percolation cluster. Dipole centers in PPX are (Tv-units of polymer chains on a surface of lamellar PPX crystallites. Such centers are characteristic, in particular, for extended polymer defects (dislocations, grain boundaries, interfaces between amorphous and crystalline areas) where, most probably, M nanoparticles are formed. [Pg.563]

Muller DA, Mills MJ (1999) Electron microscopy probing the atomic structure and chemistry of grain boundaries, interfaces and defects. Mater Sci Eng A 260 12... [Pg.289]

Clem and Fisher (1958) use a similar treatment as above to derive the solid state nucleation kinetics for new phases at grain boundaries. They neglect orientation of the critical nucleus with respect to the host, strain energy, and coherency effects. Nucleation at the grain boundary interface removes boundary energy. Their treatment yields the following critical values ... [Pg.108]

Nanophase materials feature a three-dimensional structure and a domain size of less than 100 nm. They are usually produced by compaction of a nanoscale powder and are characterized by a large number of grain boundary interfaces in which the local atomic arrangements are different from those of the crystal lattice [11.2]. Nanocomposites, in contrast, consist of nanoparticles that are dispersed in a continuous matrix, creating a compositional heterogeneity of the final structure. The matrix is usually either ceramic or polymeric. Only the manufacturing of ceramic nanocomposites applies the principles of agglomeration (Section 6.7). [Pg.1028]

Figure 17.4 Charge profiles of acceptor dopants, oxygen vacancies, and electrons near a grain boundary interface with a space charge potential of + 0.44 V, according to both the Gouy-Chapman (dotted lines) and Mott-Schottky (solid lines) models. Figure 17.4 Charge profiles of acceptor dopants, oxygen vacancies, and electrons near a grain boundary interface with a space charge potential of + 0.44 V, according to both the Gouy-Chapman (dotted lines) and Mott-Schottky (solid lines) models.
Sapphire fibers are hard, strong and scratch resistant to most materials and provide excellent wear surfaces. They can withstand higher pressures than polycrystalline alumina since they lack the grain boundary interface breakdown of the latter. Sapphire fibers transmit ultraviolet, visible, infrared and microwaves and serve as excellent wave guides between 10.6 and 17 microns, and offer durable and reliable IR transmission. By virtue of their high thermal conductivity they can be rapidly heated and cooled. [Pg.118]

Microstructure (pore, grain, surface, grain boundary, interface, etc.) X... [Pg.203]

The book begins with a review of the relevant aspects of the thermodynamics of bulk systems, followed by a description of the thermodynamic variables for surfaces and interfaces. Important surface phenomena are detailed, including wetting, crystalline systems (mcluding grain boundaries), interfaces between different phases, curved interfaces (capillarity), adsorption phenomena, and adhesion of surface layers. The later chapters also feature case studies to illustrate real-world applications. Each chapter includes a set of study problems to reinforee the reader s understanding of important concepts, with solutions available for instructors online via www.cambridge.org/meier. [Pg.241]

First, the main difference between NC and UNCD films has to be considered. The decrease of the crystal grain size from NC to UNCD films increases the number of grain boundary interfaces. This also results in a decrease of thermal conductivity and an increase of the optical absorption of UNCD films compared to NC films. At the same time, the friction coefficient of UNCD films is lower than that of NC films. Both types of CVD films can be used for MEMS (microelectromechan-ical systems), NEMS (nanoelectromechanical systems), and also for electrochemical applications. " DND is applied as an abrasive for ultrafine mechanical polishing of hard surfaces of materials. Present-day polishing compositions based on detonation ND offer the possibility of obtaining... [Pg.271]


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