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Volumn 67, Issue 14, 2003, Pages

Theory of the Shubnikov–de Haas effect in quasi-two-dimensional metals

Author keywords

[No Author keywords available]

Indexed keywords

METAL;

EID: 0038823954     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.67.144401     Document Type: Article
Times cited : (92)

References (43)
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    • D. Shoenberg, Magnetic Oscillations in Metals (Cambridge University Press, Cambridge, 1984)
    • D. Shoenberg, Magnetic Oscillations in Metals (Cambridge University Press, Cambridge, 1984).
  • 2
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    • T. Ishiguro, K. Yamaji, and G. Saito, Organic Superconductors, 2nd ed. (Springer-Verlag, Berlin, 1998)
    • T. Ishiguro, K. Yamaji, and G. Saito, Organic Superconductors, 2nd ed. (Springer-Verlag, Berlin, 1998).
  • 3
    • 85038287740 scopus 로고    scopus 로고
    • J. Wosnitza, Fermi Surfaces of Low-Dimensional Organic Metals and Superconductors (Springer-Verlag, Berlin, 1996);
    • J. Wosnitza, Fermi Surfaces of Low-Dimensional Organic Metals and Superconductors (Springer-Verlag, Berlin, 1996);
  • 6
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    • Fiz. Tverd. Tela (Leningrad) 26, 2574 (1984)
    • V. M. Gvozdikov, Fiz. Tverd. Tela (Leningrad) 26, 2574 (1984) [Sov. Phys. Solid State 26, 1560 (1984)];
    • (1984) Sov. Phys. Solid State , vol.26 , pp. 1560
    • Gvozdikov, V.M.1
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    • 0040290030 scopus 로고    scopus 로고
    • Pis’ma Zh. Éksp. Teor. Fiz. 69, 139 (1999)
    • P. Grigoriev and I. Vagner, Pis’ma Zh. Éksp. Teor. Fiz. 69, 139 (1999) [JETP Lett. 69, 156 (1999)];
    • (1999) JETP Lett. , vol.69 , pp. 156
    • Grigoriev, P.1    Vagner, I.2
  • 13
    • 23044528476 scopus 로고    scopus 로고
    • Zh. Éksp. Teor. Fiz. 119, 1257 (2001)
    • P. Grigoriev, Zh. Éksp. Teor. Fiz. 119, 1257 (2001) [JETP 92, 1090 (2001)].
    • (2001) JETP , vol.92 , pp. 1090
    • Grigoriev, P.1
  • 16
    • 0344751618 scopus 로고    scopus 로고
    • Fiz. Nizk. Temp. 27, 956 (2001)
    • V. M. Gvozdikov, Fiz. Nizk. Temp. 27, 956 (2001) [J. Low Temp. Phys. 27, 704 (2001)].
    • (2001) J. Low Temp. Phys. , vol.27 , pp. 704
    • Gvozdikov, V.M.1
  • 22
    • 85038304122 scopus 로고    scopus 로고
    • A. A. Abrikosov, Fundamentals of the Theory of Metals (North-Holland, Amsterdam, 1988)
    • A. A. Abrikosov, Fundamentals of the Theory of Metals (North-Holland, Amsterdam, 1988).
  • 36
    • 85038292319 scopus 로고    scopus 로고
    • G. Mahan, Many-Particle Physics, 2nd ed. (Plenum Press, New York, 1990), Sec. 7.1
    • G. Mahan, Many-Particle Physics, 2nd ed. (Plenum Press, New York, 1990), Sec. 7.1.
  • 37
    • 85038268573 scopus 로고    scopus 로고
    • Standard Mathematical Tables and Formulae (CRC Press, Boca Raton, FL, 1996) (or another similar book)
    • Standard Mathematical Tables and Formulae (CRC Press, Boca Raton, FL, 1996) (or another similar book).
  • 38
    • 85038306705 scopus 로고    scopus 로고
    • In the real layered compounds the impurity distribution may have a periodic modulation in the direction perpendicular to the layers, and with a period equal to the interlayer distance. However, in the Born approximation this modulation leads only to a constant factor in (11) that renormalizes the Dingle temperature
    • In the real layered compounds the impurity distribution may have a periodic modulation in the direction perpendicular to the layers, and with a period equal to the interlayer distance. However, in the Born approximation this modulation leads only to a constant factor in (11) that renormalizes the Dingle temperature.
  • 39
    • 85038336074 scopus 로고    scopus 로고
    • This fact has an evident physical meaning. The matrix element of the electron scattering by a point-like impurity U is the same for all transitions that do not change the electron energy. Hence the scattering rate (Formula presented) is proportional to the number of states to which an electron may scatter, that is, to the density of states at a given energy
    • This fact has an evident physical meaning. The matrix element of the electron scattering by a point-like impurity U is the same for all transitions that do not change the electron energy. Hence the scattering rate (Formula presented) is proportional to the number of states to which an electron may scatter, that is, to the density of states at a given energy.
  • 41
    • 85038272085 scopus 로고    scopus 로고
    • This fact can be understood in a different way: slow oscillations originate from local electron motion and are not sensitive to global variations of the position of the chemical potential with respect to the bottom of the conducting band
    • This fact can be understood in a different way: slow oscillations originate from local electron motion and are not sensitive to global variations of the position of the chemical potential with respect to the bottom of the conducting band.
  • 43
    • 0010913242 scopus 로고    scopus 로고
    • Yasunari Kurihara, J. Phys. Soc. Jpn. 61, 975 (1992)
    • Yasunari Kurihara, J. Phys. Soc. Jpn. 61, 975 (1992).


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