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19 April 2024 |
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Coupled Luttinger Liquids | | H.J. Schulz
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13 May 1996 | | Journal: | in ``Correlated Fermions and Transport in Mesoscopic Systems’’, ed. T. Martin, G. Montambaux, J. Tran Thanh Van (Editions Frontieres, Gif--sur--Yvette, 1996), p. 81. | | Subject: | cond-mat | | Affiliation: | Physique des Solides, Orsay, France | | Abstract: | Many one--dimensional quantum systems, in particular interacting electron and spin systems, can be described a Luttinger liquids. Here, some basic ideas of this picture of one--dimensional systems are briefly reviewed. I then discuss the effect of interchain coupling for a finite number of parallel chains. In the case of spin chains coupled by exchange interactions, the low--energy properties are radically different according to whether the number of coupled chains is even or odd: even number of chains have a gap in the spin excitations, whereas odd numbers of chains are gapless. The effect of interchain tunneling is analyzed for two and three coupled chains of itinerant fermions: for repulsive interactions, the two--chain system is ``universally’’ found to be a d--wave superconductor, with a gap in the spin excitation spectrum. On the other hand, for three chains the ground state depends both on the boundary conditions in the transverse direction and on the strength of the interactions. Weak repulsive interactions in all cases lead to dominant superconducting pairing of d--type. An example of a three--leg spin ladder with a spin gap is proposed. A general scheme to keep track of fermion anticommutation in the bosonization technique is developed. | | Source: | arXiv, cond-mat/9605075 | | Services: | Forum | Review | PDF | Favorites | |
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