Abstract
Chiefly simplified discussion of the (meanfield) Peieris transition; nearly-divergent density response of the 1-d conduction electron system at 2kF; its consequences for the stability of a hypothetical 1-d metal; derivation of Tc; calculation of distortion amplitude and energy gap below Tc.
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References and Footnotes
H. Fröhlich, Proc. Roy. Soc. A223, 296 (1954)
C. G. Kuper, Proc. Roy. Soc. A227, 214 (1955).
R. E. Peierls, “Quantum Theory of Solids”, (Clarendon Press, Oxford, 1955 ) p. 108.
H. R. Zeller, Festkörperprobleme 13, 31–58 (1973).
M. J. Rice and S. Strässler, Solid State Commun. 13, 125 (1973).
P. A. Lee, T. M. Rice and P. W. Anderson, Solid State Commun. 14, 703 (1974).
M. J. Rice, S. Strässler and W. R. Schneider, “Some Fluctuation and Electrodynamic Properties of the Peierls-Fröhlich Conductor”, to be published in the Proceedings of the German Physical Society Conference on “One-Dimensional Conductors”, University of Saarbrücken, 10–12 July, 1974. ( Editor H. G. Schuster).
We neglect here the periodicity of the underlying linear lattice.
See, for example, D. Pines and P. Nozières, “The Theory of Quantum Liquids, 1: Normal Fermi Liquids”, (Benjamin, New York, 1966 ).
Ref. 8, p. 237.
The mathematical structure of the mean field theory of the Peierls-Fröhlich transition is in fact identical to that of the BCS theory of the pairing superconductor (J. Bardeen, L. N. Cooper and J. R. Schrieffer, Phys. Rev. 108, 1175 (1957)).
D. Allender, J. W. Bray and J. Bardeen, Phys. Rev. B9, 119 (1974)
J. Bardeen, Solid State Commun. 13, 1389 (1973).
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Rice, M.J. (1975). Theory of the Quasi One-Dimensional Band Conductor. In: Keller, H.J. (eds) Low-Dimensional Cooperative Phenomena. NATO Advanced Study Institutes Series. Springer, Boston, MA. https://doi.org/10.1007/978-1-4899-7031-2_2
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DOI: https://doi.org/10.1007/978-1-4899-7031-2_2
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