Abstract

AbstractCoexistence of superconductivity and antiferromagnetism in low dimensional conductors can be explained by a phase segregation scenario: (i) In quasi 1D or 2D conductors in which the (T, pressure) phase diagram exhibits a border line between superconducting and spin density wave (SDW) phases, it is favourable to create a phase segregation in the direct space by forming alternatively superconducting and magnetic slabs (ii) a phase segregation may also occur in reciprocal space. A d‐wave superconducting order is established, with lines of zero gap on the Fermi surface, as in cuprates. In the node region, superconductivity is weak enough to leave room for a confined SDW gap. These models can explain consistently various recent experimental data observed in low dimensional conductors

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