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Fermi quantization effects

Surface states were also suggested to influence the diflusion of metallic adatoms on flat terraces, across atomic steps as well as the adatom detachment from the steps of nanosized metal islands [54, 55]. In the latter case, it was found that islands which, due to quantization effects, do not have a surface state at the Fermi energy (i.e., with diameters d = (n + 1), n = 0,1,2,...) are particularly stable. [Pg.155]

There are several fundamental experiments on the magnetic properties of materials that become possible as a result of the low-temperature environment of cryogenics. The first of these was discovered by deHaas and Van Alphen in 1930. They found that at low temperatures, the susceptibility of bismuth single crystals rose and fell periodically as the magnetic field was increased. Later work shows that the periodicity occurs in all metals at low temperatures and is the result of quantization of electron motion perpendicularly to the applied field. This effect was used to determine the Fermi surface of metals. [Pg.452]

It is interesting to draw a distinction between the two aspects of correlation which we have considered so far in terms of the second-quantization method for systems of N identical Fermi particles. Those methods (which are but a more effective and general way of formulating Cl) rest upon the occupation-number representation given the set of all possible single-particle states (spinorbitals), one builds a complete set of N-particle states. .. > by constructing Slater determinants or... [Pg.40]

We shall distinguish two fundamental attributes of superconductivity - the state of superconductivity and the effect of superconductivity - that lead to two complementary descriptions of superconductors. On one side the state of superconductivity is characterized by the state of a conducting material, which, after the Jahn-Teller condensation, becomes an insulator with several equivalent ground states. The state of superconductivity determines all statical properties of superconductors energy gap, its temperature dependence, specific heat, density of states near the Fermi surface etc. On the other side the effect of superconductivity determines all dynamical properties of superconductors supercurrent, Meissner effect, quantization of magnetic flux, etc. We shall devote in this section just to the problem of effect of superconductivity. [Pg.540]

The principal technique for Fermi surface analysis is the use of the de Haas-van Alphen effect. The oscillations of the magnetization of a metal in a strong magnetic field are separated from the background and analyzed into component periodicities AH. Then each periodicity so detected is directly related to an extremal cross-sectional area A of the Fermi surface, perpendicular to the applied field. The effect may be explained in terms of the quantization of the energy associated with the motion of an electron in the applied field. ... [Pg.81]


See other pages where Fermi quantization effects is mentioned: [Pg.71]    [Pg.1035]    [Pg.1035]    [Pg.115]    [Pg.515]    [Pg.54]    [Pg.1578]    [Pg.472]    [Pg.199]    [Pg.2392]    [Pg.87]    [Pg.266]    [Pg.13]    [Pg.30]    [Pg.515]    [Pg.166]    [Pg.609]    [Pg.546]    [Pg.292]    [Pg.175]   
See also in sourсe #XX -- [ Pg.279 ]




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