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Materials energies, anisotropy

The Gibbs surface free energy will usually be different for different facets of a crystal. Such variations, often referred to as surface free energy anisotropies, are key to determining the equilibrium crystal shape (as well as many other properties) of materials because at equilibrium, a crystal seeks to minimize its total surface free energy subject to the constraint of constant volume. [Pg.49]

Below a critical size the particle becomes superparamagnetic in other words the thermal activation energy kTexceeds the particle anisotropy energy barrier. A typical length of such a particle is smaller than 10 nm and is of course strongly dependent on the material and its shape. The reversal of the magnetization in this type of particle is the result of thermal motion. [Pg.176]

Definition and Uses of Standards. In the context of this paper, the term "standard" denotes a well-characterized material for which a physical parameter or concentration of chemical constituent has been determined with a known precision and accuracy. These standards can be used to check or determine (a) instrumental parameters such as wavelength accuracy, detection-system spectral responsivity, and stability (b) the instrument response to specific fluorescent species and (c) the accuracy of measurements made by specific Instruments or measurement procedures (assess whether the analytical measurement process is in statistical control and whether it exhibits bias). Once the luminescence instrumentation has been calibrated, it can be used to measure the luminescence characteristics of chemical systems, including corrected excitation and emission spectra, quantum yields, decay times, emission anisotropies, energy transfer, and, with appropriate standards, the concentrations of chemical constituents in complex S2unples. [Pg.99]

The last problem of this series concerns femtosecond laser ablation from gold nanoparticles [87]. In this process, solid material transforms into a volatile phase initiated by rapid deposition of energy. This ablation is nonthermal in nature. Material ejection is induced by the enhancement of the electric field close to the curved nanoparticle surface. This ablation is achievable for laser excitation powers far below the onset of general catastrophic material deterioration, such as plasma formation or laser-induced explosive boiling. Anisotropy in the ablation pattern was observed. It coincides with a reduction of the surface barrier from water vaporization and particle melting. This effect limits any high-power manipulation of nanostructured surfaces such as surface-enhanced Raman measurements or plasmonics with femtosecond pulses. [Pg.282]


See other pages where Materials energies, anisotropy is mentioned: [Pg.2769]    [Pg.311]    [Pg.593]    [Pg.296]    [Pg.2769]    [Pg.126]    [Pg.103]    [Pg.418]    [Pg.381]    [Pg.354]    [Pg.657]    [Pg.657]    [Pg.658]    [Pg.659]    [Pg.661]    [Pg.663]    [Pg.665]    [Pg.667]    [Pg.669]    [Pg.673]    [Pg.681]    [Pg.685]    [Pg.723]    [Pg.51]    [Pg.55]    [Pg.172]    [Pg.366]    [Pg.367]    [Pg.367]    [Pg.382]    [Pg.388]    [Pg.394]    [Pg.325]    [Pg.389]    [Pg.456]    [Pg.208]    [Pg.146]    [Pg.233]    [Pg.280]    [Pg.282]    [Pg.94]    [Pg.69]    [Pg.119]    [Pg.194]    [Pg.156]   
See also in sourсe #XX -- [ Pg.480 ]




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Anisotropy energy

Anisotropy materials

Surface energy anisotropy in strained materials

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