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The Fermi Surface

2007
At 0 K the normal metal has a sharp Fermi surface, which is experimentally supported by the fact that the heat capacity is linear in the temperature T at the lowest temperatures. The Fermi surfaces in a few metals are discussed in this chapter.
Kei Ito, Shigeji Fujita
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Fermi surface oF CeSn3

Physica B: Condensed Matter, 1990
Abstract Based on an itinerant model for the 4f electrons, the energy band structure is calculated for CeSn3, known to be the heavy-electron system having the Kondo temperature of about 200 K, by a self-consistent relativistic APW method with the exchange and correlation potential in the local-density approximation.
Hiroshi Yamagami, Akira Hasegawa
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Fermi Surface of Tellurium

physica status solidi (b), 1970
AbstractA study of the Shubnikov‐de Haas effect allowed us to determine the Fermi surface of tellurium. At low impurity concentration, the Fermi surfaces are ellipsoidal. When the impurity concentration increases, the ellipsoids coalesce and form a dumb‐bell surface. For p ≈ 1.5 × 1017 cm−3, the ellipsoids are just joining together.
J. M. Thuillier, C. Guthmann
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The Fermi surface of CeRu2Si2

Journal of Magnetism and Magnetic Materials, 1992
Abstract A comparison of the Fermi surface calculated by a relativistic APW method and the local-density approximation with the de Haas-van Alphen effect observed in the heavy-electron system CeRu 2 Si 2 shows that the 4f electrons may not be itinerant in its ground state.
Akira Hasegawa, H. Yamagami
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The Fermi Surfaces of Metals

Nuclear Technology, 1972
A P Cracknell London: Taylor and Francis 1971 pp 283 price £3.50 This book is the latest in a series of Monographs on Physics and combines in a single volume the two parts of a review which originally appeared in Advances in Physics. The book gives an account of the Fermi surface shapes of metals and reviews the relevant experimental and theoretical ...
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The Fermi Surface of Graphite

IBM Journal of Research and Development, 1964
Recent magnetoreflection measurements in pyrolytic graphite have been interpreted using the magnetic energy levels obtained from the McClure-lnoue secular equation and the appropriate selection rules for interband transitions. Combining these results with those of the de Haas - van Alphen effect, the band parameters of the Slonczewski-Weiss model have ...
Mildred S. Dresselhaus, J. G. Mavroides
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The Fermi surface of aluminium

Physics Letters, 1963
Abstract The de Haas–van Alphen data in aluminium are compared with periods arising from extremal sections on a Fermi surface defined by a fourth-order secular equation. The Fourier coefficients V 111 and V 200 of the weak pseudopotential are regarded as adjustable parameters.
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Fermi surface of LaAg

Zeitschrift f�r Physik B Condensed Matter, 1995
Electronic structure, especially the Fermi surface, is calculated for the intermetallic rare-earth compound LaAg, known to show the structural phase transition when In is substituted for Ag, by a self-consistent fully-relativistic APW method with the exchange-correlation potential in a local-density approximation.
Masahiko Higuchi, A. Hasegawa
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The Fermi surface of beryllium

Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences, 1963
The Fermi surface of beryllium has been determined experimentally by studying the de Haas–van Alphen effect of single crystals in pulsed magnetic fields. The de Haas–van Alphen frequency (proportional to the extremal area of the Fermi surface normal to the field) was measured as a function of field direction.
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Fermi Surface of Ni

Journal of the Physical Society of Japan, 1964
The energy band structure of ferromagnetic nickel is evaluated by the Green's function method and the interpolation method developed by Slater and Koster. The effective potential is suitably chosen so as to give a reasonable fit with the results of recent experiments about the Fermi surface.
Jiro Yamashita, Shinya Wakoh
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