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Superconductivity through Quantum Critical Fluctuations in the ...

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s but simply characterized temperaturerties studied. Characteristic Fermi-liquidregion (II) an anisotropic gap (pseudoicalpotential is observed. Transport [?]racteristic changes below <strong>the</strong> l<strong>in</strong>e T p (x).erties across di erent l<strong>in</strong>es also occur. Itnd <strong>the</strong> universal properties.Experiments consistent with this long-range order.This order has been observed <strong>in</strong> four dist<strong>in</strong>ct families ofCuprates by Polarized Neutron scatter<strong>in</strong>g or by DichroicARPES.YBa(2)Cu(3)O(6+x)Bi2212HgBaCuOLSCO:IIIFermi liquidCrossoverx (dop<strong>in</strong>g)Temperature (K)4003002001000T (K)and discussed fur<strong>the</strong>r belowHg1201 are <strong>in</strong> good agreem400 <strong>in</strong> Figs. 1-5 demonstrate tha300netic signal belowysis method.T mag is <strong>in</strong>It is fur<strong>the</strong>rm200100crease of T ⇤ toward higher hoappearance of <strong>the</strong> pseudogapdop<strong>in</strong>g. Moreover, as alread00.05 0.1 0.15 0.2p0.05 0.1 0.15 0.2Hole dop<strong>in</strong>g player YBCO. 3,4,9 . These releast <strong>in</strong> compounds with higpseudogap phenomenon is aa mere crossover.In Ref. 4 an attempt wascal exponent of <strong>the</strong> transitiothat <strong>the</strong> fit value depends otr<strong>in</strong>sic temperature dependenconsidered <strong>in</strong> comparisons wof 2 =0.37±0.12 is consiste5). The uncerta<strong>in</strong>ty <strong>in</strong> <strong>the</strong>

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