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      Probing the Gauge Structure of high-temperature superconductors

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          Abstract

          We suggest that a spin-charge separating ansatz, leading to non-Abelian \(SU(2) \otimes U_S(1)\) gauge symmetries in doped antiferromagnets, proposed earlier as a way of describing Kosterlitz-Thouless superconducting gaps at the nodes of the gap of d-wave (high-T_c) superconductors, may also lead to a pseudogap phase, characterised by the formation of (non-superconducting) pairing and the absence of phase coherence. The crucial assumption is again the presence of electrically charged Dirac fermionic excitations (holons) about the points of the (putative) fermi surface in the pertinent phase of the superconductor. We present arguments in support of the r\^ole of non-perturbative effects (instantons) on the onset of the pseudogap phase. As a means of probing such gauge interactions experimentally, we perform a study of the scaling of the thermal conductivity with an externally-applied magnetic field, in certain effective models involving gauge and/or four-fermion (contact) interactions.

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          Catalysis of Dynamical Flavor Symmetry Breaking by a Magnetic Field in 2+1 Dimensions.

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            Critical Behavior in (2+1)-Dimensional QED

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              SU(2) gauge symmetry of the large-Ulimit of the Hubbard model

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                Author and article information

                Journal
                29 May 1998
                1998-06-04
                Article
                10.1142/S0217979298001459
                cond-mat/9805402
                ca3943ed-f7a4-4862-99bc-6763f82e46f5
                History
                Custom metadata
                NTUA-71/98, OUTP-98-43P
                Int.J.Mod.Phys. B12 (1998) 2475-2494
                27 pages LATEX, six figures incorporated (minor typos and cosmetic changes)
                cond-mat hep-lat hep-ph

                Condensed matter,High energy & Particle physics
                Condensed matter, High energy & Particle physics

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