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Thermal interaction with material

Hassan, M. M., Badway, N. A., Gamal, A. M., Elnaggar, M. Y, Hegazy E.-S. A., Studies on mechanical, thermal and morphological properties of irradiated recycled polyamide and waste rubber powder blends. Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms 2010, 268, 1427-1434. [Pg.300]

Borionetti, G., Geranzani, P, Orizio, R., Godio, P, Bonoh, E, Pagani, E, PeUo, C. (2006) Metal and organic contamination effects on the characteristics of thin oxides thermally grown on silicon based wafers. Nuclear Instruments and Methods in Physics Research Section B Beam Interactions with Materials and Atoms, 253, 278-281. [Pg.929]

The second class of atomic manipulations, the perpendicular processes, involves transfer of an adsorbate atom or molecule from the STM tip to the surface or vice versa. The tip is moved toward the surface until the adsorption potential wells on the tip and the surface coalesce, with the result that the adsorbate, which was previously bound either to the tip or the surface, may now be considered to be bound to both. For successful transfer, one of the adsorbate bonds (either with the tip or with the surface, depending on the desired direction of transfer) must be broken. The fate of the adsorbate depends on the nature of its interaction with the tip and the surface, and the materials of the tip and surface. Directional adatom transfer is possible with the apphcation of suitable junction biases. Also, thermally-activated field evaporation of positive or negative ions over the Schottky barrier formed by lowering the potential energy outside a conductor (either the surface or the tip) by the apphcation of an electric field is possible. FIectromigration, the migration of minority elements (ie, impurities, defects) through the bulk soHd under the influence of current flow, is another process by which an atom may be moved between the surface and the tip of an STM. [Pg.204]

Fast neutrons rapidly degrade in energy by elastic collisions when they interact with low atomic number materials. As neutrons reach thermal energy, or near thermal energies, the likelihood of capture increases. In present day reactor facilities the thermalized neutron continues to scatter elastically with the moderator until it is absorbed by fuel or non-fuel material, or until it leaks from the core. [Pg.33]

PALS is based on the injection of positrons into investigated sample and measurement of their lifetimes before annihilation with the electrons in the sample. After entering the sample, positron thermalizes in very short time, approx. 10"12 s, and in process of diffusion it can either directly annihilate with an electron in the sample or form positronium (para-positronium, p-Ps or orto-positronium, o-Ps, with vacuum lifetimes of 125 ps and 142 ns, respectively) if available space permits. In the porous materials, such as zeolites or their gel precursors, ort/zo-positronium can be localized in the pore and have interactions with the electrons on the pore surface leading to annihilation in two gamma rays in pick-off process, with the lifetime which depends on the pore size. In the simple quantum mechanical model of spherical holes, developed by Tao and Eldrup [18,19], these pick-off lifetimes, up to approx. 10 ns, can be connected with the hole size by the relation ... [Pg.42]

The assessment begins with an assessment of the reactants. The question is whether all initial process reactants can be regarded as thermally stable within the intended temperature range and time domain. Possible interactions with non-reacting materials need to be considered as part of this assessment. [Pg.235]


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See also in sourсe #XX -- [ Pg.320 ]




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