ar X iv : c on d - m at / 9 50 71 24 v 1 2 7 Ju l 1 99 5 Intercalation and Staging Behavior in Super - Oxygenated

ar X iv : c on d - m at / 9 50 80 62 v 1 3 1 Ju l 1 99 5 QUANTUM THEORY OF LARGE SYSTEMS OF NON - RELATIVISTIC MATTER

ar X iv : c on d - m at / 9 50 71 21 v 1 2 7 Ju l 1 99 5 Exact Critical Exponents for Pseudo - Particles in the Kondo Problem

Exact critical exponents of the Green functions for pseudo-fermions and slave bosons in the SU(N) Anderson model with U → ∞ are obtained by using the Bethe ansatz solution and boundary conformal field theory. They are evaluated exactly for mixed valence systems and Kondo systems with crystalline fields. The results agree with the prediction of Menge and Müller-Hartmann, which coincide with thos...

ar X iv : c on d - m at / 9 50 71 07 v 1 2 5 Ju l 1 99 5 Two interacting particles in an effective 2 - 3 – d random potential

We study the effect of coherent propagation of two interacting particles in an effective 2-3-d disordered potential. Our numerical data demonstrate that in dimension d > 2, interaction can lead to two–particles delocalization below one–particle delocalization border. We also find that the distance between the two delocalized particles (pair size) grows logarithmically with time. As a result pai...

ar X iv : a lg - g eo m / 9 70 70 16 v 1 2 5 Ju l 1 99 7 RATIONAL CURVES ON QUASI - PROJECTIVE SURFACES

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ar X iv : c on d - m at / 9 50 70 89 v 2 3 1 Ju l 1 99 5 Is there a renormalization of the 1 D conductance in Luttinger Liquid model ?

Properties of 1D transport strongly depend on the proper choice of boundary conditions. It has been frequently stated that the Luttinger Liquid (LL) conductance is renormalized by the interaction as g e 2 h. To contest this result I develop a model of 1D LL wire with the interaction switching off at the infinities. Its solution shows that there is no renormalization of the universal conductance...