Galvanomagnetic and thermomagnetic effects in compensated gallium arsenide
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Abstract
The kinetic effects:-Hall effect, magnetoresistance, and Nernst-Ettinghausen effect-are examined in n-type gallium arsenide having a free electron concentration at room temperature of less than 1015 cm−3.
The work was directed toward determining the dominating scattering mechanism in compensated material.
At low temperatures the scattering is predominately by impurity atoms and optical vibrations (optical phonons); at high temperatures, by acoustic phonons.
With simultaneous scattering by thermal vibrations and impurity ions, for temperatures T > 300 ° K, the second mechanism plays the basic role in the longitudinal Nernst-Ettinghausen effect.
Keywords
Gallium Electron Concentration Free Electron Hall Effect Impurity Atom
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References
- 1.O. V. Emel'yanenko and D. N. Nasledov, ZhTF28, no. 6, 1177, 1958.Google Scholar
- 2.O. V. Emel'yanenko and D. N. Nasledov, FTT,1, no. 6, 985, 1959.Google Scholar
- 3.O. V. Emel'yanenko, T. S. Lagunova, and D. N. Nasledov, FTT,2, no. 2, 192, 1960.Google Scholar
- 4.D. N. Nasledov, J. Appl. Phys. Suppl. to vol. 32, no. 10, 2140, 1961 (Transactions of Conference on Semiconducting Compounds, Schenectady, New York, 1961).Google Scholar
- 5.A. F. Kravchenko, Izv. VUZ. Fizika, no. 3, 80, 1961.Google Scholar
- 6.R. Barrie, F. A. Cunnell, J. T. Edmond, and I. M. Ross, Physica,20, no. 11, 1087, 1954.Google Scholar
- 7.L. Pincherle and J. M. Radcliffe, Collection: Advances in Physics,5, no. 19, p. 271, 1956.Google Scholar
- 8.A. F. Kraychenko and H. Y. Fan, FTT,5, no. 2, 660, 1963.Google Scholar
- 9.J. W. Allen, Nature, 187, no. 4735, 403, 1960.Google Scholar
- 10.C. Hilsum and A. C. Rose-Innes, Semiconducting III-V Compounds, N. Y.-London, 1961.Google Scholar
- 11.C. H. Gooch, C. Hilsum, and B. R. Holeman, J. Appl. Phys., Suppl. to vol. 32, no. 10, 2069, 1961.Google Scholar
- 12.L. R. Weisberg, F. D. Rosi, and P. G. Herkart, collection: Properties of Elemental and Compound Semiconductors (Metallurgical Society Conference, Boston, 1959, V. 5), New York, p. 25, 1960.Google Scholar
- 13.J. M. Whelan and G. H. Wheatley, J. Phys. Chem. Solids,6, nos. 2–3, 169, 1958.Google Scholar
- 14.H. Brooks, Collection: Advances in Electronics and Electron Physics, vol. 7, New York, p. 85, 1955.Google Scholar
- 15.L. R. Weisberg, F. D. Rosi, and P. G. Herkart, collection: Properties of Elemental and Compound Semiconductors (Metallurgical Society Conference, Boston, 1959, vol. 5), New York, p. 85, 1960.Google Scholar
- 16.L. R. Weisberg, J. R. Woolston, and M. Glicksman, J. Appl. Phys., 29, no. 10, 1514, 1958.Google Scholar
- 17.E. M. Conwell and V. F. Weisskopf, Phys. Rev.,77, no. 3, 388, 1950.Google Scholar
- 18.K. B. Tolpygo, Trudy instituta fiziki AN USSR, 3, 52, 1952.Google Scholar
- 19.I. M. Tsidil'kovskii, Thermomagnetic Phenomena in Semiconductors [in Russian], Fizmatgiz, Moscow, 1960.Google Scholar
- 20.H. Ehrenreich, Phys. Rev., 120, no. 6, 1951, 1960.Google Scholar
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