2 research outputs found
Microscopic theory of the pseudogap and Peierls transition in quasi-one-dimensional materials
The problem of deriving from microscopic theory a Ginzburg-Landau free energy
functional to describe the Peierls or charge-density-wave transition in
quasi-one-dimensional materials is considered. Particular attention is given to
how the thermal lattice motion affects the electronic states. Near the
transition temperature the thermal lattice motion produces a pseudogap in the
density of states at the Fermi level. Perturbation theory diverges and the
traditional quasi-particle or Fermi liquid picture breaks down. The pseudogap
causes a significant modification of the coefficients in the Ginzburg-Landau
functional from their values in the rigid lattice approximation, which neglects
the effect of the thermal lattice motion. To appear in Physical Review B.Comment: 21 pages, RevTeX, 5 figures in uuencoded compressed tar fil
Ginzburg-Landau theory of phase transitions in quasi-one-dimensional systems
A wide range of quasi-one-dimensional materials, consisting of weakly coupled
chains, undergo three-dimensional phase transitions that can be described by a
complex order parameter. A Ginzburg-Landau theory is derived for such a
transition. It is shown that intrachain fluctuations in the order parameter
play a crucial role and must be treated exactly. The effect of these
fluctuations is determined by a single dimensionless parameter. The
three-dimensional transition temperature, the associated specific heat jump,
coherence lengths, and width of the critical region, are computed assuming that
the single chain Ginzburg-Landau coefficients are independent of temperature.
The width of the critical region, estimated from the Ginzburg criterion, is
virtually parameter independent, being about 5-8 per cent of the transition
temperature. To appear in {\it Physical Review B,} March 1, 1995.Comment: 15 pages, RevTeX, 5 figures in uuencoded compressed tar file