By E. Fawcett, R. Griessen, W. Joss, W. Kress
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Additional info for Phonon States of Alloys. Electron States and Fermi Surfaces of Strained Elements
P;‘“. , . :: : .... 1 .. T Fig. 1. a-Be. Representative extremal cross sections of the Fermi surface [67Cl, 69Tl]. 2. 3 Electron states of strained elements: Ba, Be Ref. p. 2481 Fig. 1. Ba. Energy bands plotted as a function of volume Q is obtained from an ASA calculation. Td, C,, B, are the top, :entre and bottom of the d band, C, the centre of the f band, B, the bottom of the s band, @is the potential at the atomic sphereradius R,, [78Dl]. 5808, (T=75 K) BZ: seep. 450of Vol. III/13a 1. , .
BZ: see p. 449 of Vol. 6 0 2 4 6p; 10 12 GPa 14 Fig. 7. a-As. Relative change of the concentration of current carriers with hydrostatic pressure obtained from a measurement of the transverse magnetoconductivity as a function of pressure (pressure medium: solid oil-kerosene or pyrophyllite) [80Rl]. 1. Fermi surface Au Fig. 1. Au. Representative extremal cross sections of the Fermi surface (seeFig. 1 Ag). Joss/Griessen/Fawcett 31 Ref. 0 N Fig. 6. a-As. 5 pressure (pressure medium: solid oil-kerosene or AgCl) P[68B3].
40 P- t Fig. 14. Bi. Smallest extremal cross-sectional area of the electron surface (A, C) with magnetic field parallel to the [llTO]-binary axis as a function of hydrostatic pressure. The shaded area denotes the estimated uncertainty in the initial slope as determined by the fluid He phase shift DHVA work. The dots being the results of the solid He pressure technique [7OS3]. 4 P- Fig. 15. Bi. Hydrostatic pressuredependenceof the frequency of the Shubnikov-de Haas oscillations of the electron pocket (A) with the magnetic field parallel to the [lOiO]bisectrix axis (pressure medium: solid oil-kerosene).