Titlebook: Surface Modification and Alloying; by Laser, Ion, and E J. M. Poate,G. Foti,D. C. Jacobson Book 1983 Springer Science+Business Media New Yo

性满足

载货清单

Crystal Growth and Phase Formation,by the motion of an interface between them. The interface can traverse the sample substantially at a single temperature and so the finite heat which is released at this temperature results in an infinite specific heat. By contrast, transformations of higher orders are, in general, homogeneous in spa

极为愤怒

Segregation, Supersaturated Alloys and Semiconductor Surfaces, to a depth of several thousand angstroms, followed by liquid phase epitaxial regrowth from the underlying substrate (Ferris ., 1979; White and Peercy, 1980; Gibbons ., 1981; Appleton and Celler, 1982). In silicon, the velocity of the liquid-solid interface during solidification is calculated (Wang

SNEER

Solid Phase Recrystallization Processes in Silicon, treatment. The recrystallization process usually proceeds epitaxially on the underlying crystalline silicon substrate via either liquid or solid phase processes depending on the annealing procedure adopted. The previous chapter treated the annealing behavior during intense and rapid (nsec) laser or

启发

Metastable Alloys and Superconductivity,materials with special properties which cannot be met using standard equilibrium growth methods. In addition many applications require this special material only in the near surface region, whereas the bulk properties of the material should not be affected. In order to meet these different requireme

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Collision Cascades and Spike Effects,ributed over ~0.5 .m depth) is of the order of 1-2 eV/atom and the quenching time .. for the resulting molten zone is ~10. seconds. There are at least three ways in which . beams may be used to achieve comparable energy densities and quench rates (Table I):

Arteriography

Solute Redistribution and Precipitate Stability: Point-Defect Mediated Effects,their sites in a crystalline solid by energetic collisions, and the point defects can diffuse if the temperature is sufficiently high. Defect migration allows atomic diffusion. In this chapter the consequences of the atomic diffusion due to the migration of irradiation-produced point defects will be

傲慢物

Ion Beam Mixing,tion. Due to these changes, material properties of the system may be modified in ways sometimes difficult to achieve by conventional methods. From a collisional point of view, ion beam mixing effects result from particle-solid interactions. The phenomena become more complex when thermodynamical forc

Irritate

Sputtering and Compositional Changes,). However, most of the present experimental knowledge and theoretical understanding of the sputtering phenomenon has been gained during the past 30 years. Extensive, recent reviews of many aspects of the sputtering phenomenon can be found in volumes edited by Varga . (1980), by Cobic (1980), and by

Inflamed

Surface Modification and Alloying: Aluminum,ys independently of the usual equilibrium constraints. A variety of such surface modification studies have recently been carried out in aluminum by several groups (Battaglin ., 1981; Hussain . Peercy ., 1982; and Picraux ., 1980. Selected results from these studies are summarized in the present chap