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Fermiliquid 266 -inTl2Ba2CaCu2Os 255 -in La2.x(Sr)xCuO4 I 19 Fluctuation effects -in TIBa2Ca2Cu309 255 -in YBa2Cu408 75 -inYiBa2Cu307 449 -in YBCO II Coherence length Flux creep Irreversibility field 140 -in YiBa2Cu307 449 -in Bi2Sr2CaCu2Os 140 Composition determination by -in YBa2Cu3OT_6 140 Lattice dynamics EPMA 365 Flux dynamics 161,225 -ofYBa2Cu3OT_6 225 Criticalcurrent density ll, 41, 64, 203 -inTl2Ba2Ca2Cu3Ox 456 LayeredHTSCs 161 -in Dy~Ba2Cu307_6 89 Fluxlattice 51 Low frequency impedance 275 -in La2.x(Sr)xCuO 4 ll9 -inTl2Ba2Ca2Cu3Ox 456 Luttingerliquid 266 -in YBa2Cu3Ov_x wires 81 Flux pinning 11, 41 -inYBa2Cu3Ox 147 -in YBa2CuaO7_6 225 Magnetic susceptibility 301 -in Y-Ba-Cu-O 411 -inYBa2Cu3Ox 147 -ofBi2SrzCan_lCunO2.+4 231 Criticalphenomena Flux pinning, enhancement of 255 -ofBi2Sr2CuO~6 ll0 -ofLa2_x(Sr)xCuO4 ll9 Fullerene 137 -of x-(BEDT-TTF)zCu(NCS)2 Cu K edge 324 -ofYBa2Cu3OT_n 37 -ofCu20 352 Ginzburg-Landautheory 51 Magnetization -ofCuO 352 y-irradiationeffect 11 -in Bi2Sr2Cal_xYxCu2Os+6 432 -of La2CuO4 421 Grain alignment (texturing) 147 -of Bi2Sr2CaCu2Os 140 -ofYBa2Cu3OT_y 352 Granular superconductivity -ofGdBa2Cu3OT_6single crystal Cu L3 edge -in (Bi, -ofNd2CuO4 189 -ofLa2CuO4 421 Pb)2+xSr2_yCa2+yCu3+~Olo+a 203 -ofYBa2Cu3OT_6 140
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