The fermi surface in white tin

Gold, A.; Priestley, M. G.

doi:10.1080/14786436008238318

Cited by 62 publications

(6 citation statements)

References 9 publications

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“…strain of extremal orbits on all sheets of the Fermi Measurements of extremal cross-sectional areas of surface of tin. Derivatives of area with respect to the Fermi surface have been using both con-strain both along the (loo) axes in the tetragOnal ventional de Haasvan Alphen (dHvA) oscillations crystal, and along the [0011 tetrad axis, have been (1)(2)(3) and quantum oscillations in ultrasonic found for eight orbits normal to [OOlI, five normal attenuation (4)(5)(6); Fermi surface calipers have been to [loo], and four normal to [ll01. In additi0n, strain measured using the radio frequency size effect derivatives have been determined for three branches (7)(8)(9)(10).…”

Section: Introductionmentioning

confidence: 99%

Experimental determination of the dilational strain dependence of the Fermi surface of white tin

Mak¹,

Perz²

1980

Can. J. Phys.

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The derivatives with respect to uniaxial elongational strain of the areas of representative orbits on all sheets of the Fermi surface of tetragonal white tin have been deduced from simultaneous measurements of the Landau quantum oscillations in elastic moduli and in torque. Strain derivatives have been determined for most known extremal cross-sectional areas normal to the [100], [110], and [001] symmetry axes; the anisotropy of the strain derivatives of several area branches, having normal directions in the (010) and (001) planes, has also been studied. Uniaxial and hydrostatic stress derivatives deduced from the strain derivatives have been found to be generally consistent with values obtained by other means.

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Section: Introductionmentioning

confidence: 99%

Experimental determination of the dilational strain dependence of the Fermi surface of white tin

Mak¹,

Perz²

1980

Can. J. Phys.

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“…Here we get ahead of the interpretation in thc next chapter. The notation of Gold and Priestley [8] and Gantmakher [l] is used as much as possible : a number, the zone number, is followed by a Greek letter, which denotes the type of orbit. If an orbit has no equivalent in Gold's construction, only the zone number is mentioned.…”

Section: Resultsmentioning

confidence: 99%

The Fermi Surface of White Tin from RF Size Effect Measurements

Matthey

Devillers

Vroomen

1974

Physica Status Solidi (b)

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“…For g # 0, U(g) can be approximated by the ionic pseudopotential screened by the dielectric constant ~d ( g ) (51, as [I31 U(g) = UiO" (g)le,(g) Its energy dependence is given by [I41 dU(g)ldE1 = (l/&,(g)) (dUiO"(g)ldE') dUiOn(g)/d~' can be calculated froin [lo], [ll], and [12]. The dielectric constants for tin have been calculated by Mak and Perz (3).…”

Section: Band Massmentioning

confidence: 99%

The determination of band masses and deformation potentials in white tin from an orthogonalized plane wave pseudopotential model

Mak¹

1980

Can. J. Phys.

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A method for calculating band masses. using an orthogonalized plane wave (OPW) formalism and taking into account the energy dependence of the pseudopotential form factors, is derived. This is applied to white tin; the results prove to be sensitive only to the energy dependence of the lowest form factor. Deformation potentials for various orbits have been calculated; they are found to be quite anisotropic over the Fermi surface.On etablit une methode pour le calcul des masses de bandes qui utilise un formalisme OPW et qui tlent compte de la variation des facteurs de forme du pseudo-potentiel en fonction de I'energie. Cette rnethode est appliquee a I'etain blanc; les resultats apparaissent sensibles uniquement a la variation du plus bas facteur de forme en fonction de l'energie. Des potentiels de deformation ont ete calcules pour differentes orbites, et on trouve qu'ils sont fortement anisotropes sur l'etendue de la surface de Fermi.[Traduit par le journal]Can. J. Phys.. 1040(1980)Introduction various calculations. He noted that the energy The dynamical properties of electron quasiparticle dependence of the one-electron potential Parameters excitations in a metal are affected by both electron-had been ignored in earlier calculations of band phonon and electron-electron interactions. The masses.the augmented plane wave (APW) quasi-particle cyclotron effective mass IH,,, which is method, he calculated values of m, for a number of determined from experiment can be expressed in orbits in tin taking into account the energy depenterms of a 'bare' band mass n z b , and renormalization dence of a,, the logarithmic derivatives of the I-deparameters A,, and A,,, referring to electron-phonon pendent radial function of the muffin-tin potential at and electron-electron interactions, respectively, as the muffin-tin radius; the are the Parameters describing the Fermi surface in the APW formalism. nzexp = In,o

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The fermi surface in white tin

Cited by 62 publications

References 9 publications

Experimental determination of the dilational strain dependence of the Fermi surface of white tin

Experimental determination of the dilational strain dependence of the Fermi surface of white tin

The Fermi Surface of White Tin from RF Size Effect Measurements

The determination of band masses and deformation potentials in white tin from an orthogonalized plane wave pseudopotential model

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