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Deformation-potential interaction, effective

Equation (102) shows that MAQO can provide important information about the electronic parameters (extremal Fermi surface cross-sectional area, effective masses, electronic relaxation times) and about the electron-phonon interaction (strain derivatives of the cross-sectional area for different symmetry strains). With the help of this technique, combined with de Haas-van Alphen susceptibility measurements, one can put the deformation potential interaction and the temperature dependence of the elastic constants, discussed above in sect. 3.2, on a solid basis. In the following we discuss some compounds. [Pg.293]

At high enough electrolyte concentrations the electric potentials are quickly dissipated and this effect vanishes. Since droplets and bubbles are not rigid spheres, they may deform in shear flow. Also, with the presence of emulsifying agents at the interface, the drops will not be non-interacting, as is assumed in the theory. [Pg.31]


See other pages where Deformation-potential interaction, effective is mentioned: [Pg.537]    [Pg.217]    [Pg.65]    [Pg.297]    [Pg.744]    [Pg.306]    [Pg.327]    [Pg.179]    [Pg.327]    [Pg.223]    [Pg.230]    [Pg.391]    [Pg.459]    [Pg.110]    [Pg.705]    [Pg.461]    [Pg.337]    [Pg.219]    [Pg.85]    [Pg.209]    [Pg.101]    [Pg.26]    [Pg.91]    [Pg.133]    [Pg.78]    [Pg.132]    [Pg.125]    [Pg.185]    [Pg.453]    [Pg.47]    [Pg.111]    [Pg.38]    [Pg.70]    [Pg.423]    [Pg.238]    [Pg.9]    [Pg.185]    [Pg.194]    [Pg.405]    [Pg.311]    [Pg.62]    [Pg.399]    [Pg.267]    [Pg.230]    [Pg.405]    [Pg.47]    [Pg.78]    [Pg.1309]   
See also in sourсe #XX -- [ Pg.391 , Pg.459 ]




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