Interaction of Charged Particles and Atoms with Surfaces by G. Chiarotti (auth.), G. Chiarotti (eds.)

By G. Chiarotti (auth.), G. Chiarotti (eds.)

Surface physics has skilled within the final many years an explosive growth brought on by the improvement and/or great development of floor delicate innovations and UHV apparatuses. It has grown right into a mature box of study, with information of the top accuracy and reproducibility. floor physics is of serious value for technological purposes like box influence units, molecular beam epitaxy, chemisorption and catalysis, corrosion, floor hardening and so on. the current volume III/24 is specific to the so-called "clean" surfaces, i.e. to surfaces atomically fresh and good characterised, leaving the extra advanced box of the tainted surfaces and overlayers to a later occasion.

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Extra resources for Interaction of Charged Particles and Atoms with Surfaces

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This system enables measurements to be made at very high angles of incidence [72G3, 74A1, 74Dl], and very precise and reproducible conditions of incidence are reached by means of an external two-circle goniometer. A similar apparatus was also built in York [84D2]. For this kind of system a special miniaturized gun was designed [82Cl]. The use of polarized electrons for surface studies requires special sources and/or detectors. When a primary polarized beam is necessary, sources such as those used in atomic physics are not very convenient as they involve atomic beams and they are consequently difficult to use under UHV conditions [76Kl, 8OCl].

88 “experimental” delta functions [74A2, 74L1, 75A2, 75L2, 77A1, 79A2, 791112,79M33 or one can directly try to obtain directly agreement between the experimental transform and a trial kinematic transform by minimizing an appropriate mean distance between the two curves (called residual) [77C6, 78C1, 78C2]. In any case, the above methods are to be taken as simply indicative, and they may be useful permitting the possible exclusion of a model. 2 Simplifications and calculations As the main method for obtaining information about atom positions remains full dynamical calculation, many simplifications were introduced to shorten the computer time and core requirements.

Finally, in the last decade LEPD has been attempted, and very recently some aspects of this technique showed it to be an important rival of LEED for surface crystallography. Because of the wide interest and diffusion of electron diffraction several books are now available on this subject [74P, 79V, 85C, 85K2, 86Vl] and a large number of review articles can be found in the literature [88J4]. In the following sections, the physical principles, the existing theories, instrumentation and experimental particulars and the reliability and precision of the above mentioned techniques will be briefly and schematically reviewed with the aim of providing a wide bibliographical basis for each topic.

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