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It is shown that in the framework of a generalised Ginzburg-Landau scheme based on the microscopic model of chains of 1D Fermi gases interacting via a Coulomb-type interaction it is possible to account for the observed critical behaviour near the 53K phase transition of TTF-TCNQ. The pseudogap is also calculated and its effect on the electronic density of states is found to disappear above the critical region.
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N. Menyhárd (1979) studied this question.
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