The effective mass of electrons in (InSb) x ·(InTe) 1−x  crystals | Zendy

Molodyan I. P. | Zendy; Nasledov D. N. | Zendy; Radautsan S. I. | Zendy; Sidorov V. G. | Zendy

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The effective mass of electrons in (InSb) x ·(InTe) 1−x crystals

Author(s) -

Molodyan I. P.,

Nasledov D. N.,

Radautsan S. I.,

Sidorov V. G.

Publication year - 1966

Publication title -

physica status solidi (b)

Language(s) - English

Resource type - Journals

SCImago Journal Rank - 0.51

H-Index - 109

eISSN - 1521-3951

pISSN - 0370-1972

DOI - 10.1002/pssb.19660180219

Subject(s) - solid solution , seebeck coefficient , tellurium , electron , effective mass (spring–mass system) , condensed matter physics , doping , hall effect , atmospheric temperature range , thermoelectric effect , chemistry , conductivity , electrical resistivity and conductivity , nernst effect , materials science , analytical chemistry (journal) , nernst equation , physics , thermodynamics , inorganic chemistry , nuclear physics , electrode , quantum mechanics , chromatography , organic chemistry

Measurements of the thermoelectric power, transverse Nernst‐Ettinghausen effect, conductivity, and Hall effect allow the concentration and temperature dependence of the electronic effective mass m * to be calculated for crystals of the solid solution (InSb) x (InTe) 1—x (for × = 1 to 0.85) in the temperature range 100 to 370 °K. Solid solutions having × > 0.99 (I) behave like InSb doped with tellurium, and crystals of this type having electron concentrations ( n ) greater than 2 × 10 18 cm −3 show an m * ( n ) dependence which differs from that predicted by Kane. Solid solutions with x ≦ 0.99 (II) show a different temperature dependence of m * from those with x > 0.99.

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