E. Galstyan

Possible origin of the higher magnetic phase transition in RuSr2Eu1.5Ce0.5Cu2O10

{\mathrm{Eu}}_{2\ensuremath{-}x}{\mathrm{Ce}}_{x}{\mathrm{RuSr}}_{2}{\mathrm{Cu}}_{2}{\mathrm{O}}_{10\ensuremath{-}\ensuremath{\delta}}

Tuning the superconducting state in the magnetic MoSr 2 YCu 2 O 8 − δ materials

(Ru-2122) is the first Cu-O-based system in which superconductivity (SC) in the

Magnetism and Superconductivity in RuM1.5Ce0.5Sr2Cu2O10 (M=Eu and Y)

{\mathrm{CuO}}_{2}

Magnetization andFe57andSn119Mössbauer studies of magnetism inRuR2−xCexSr2Cu2O10(R=Eu,Gd)

planes and weak ferromagnetism (WFM) in the Ru sublattice coexist. The hole doping in the

Evolution of core connectivity in MgB2 wires and tapes during PIT processing

{\mathrm{CuO}}_{2}

Reply to “Comment on ‘Origin of the superconductivity in the Y-Sr-Ru-O and Y-Sr-Cu-O systems’ ”

planes is controlled by appropriate variation of the Ce concentration. SC occurs for Ce contents of 0.4\char21{}0.8, with the highest

Micro-structure and magnetization of the 80-K superconductor, TbSr2Cu2.7Mo0.3O7+δ

{T}_{C}=35\mathrm{K}

Magnetization and Fe57 and Sn119 Mssbauer studies of magnetism in RuR2-xCexSr2Cu2O10 (R=Eu,Gd)

for

Magnetization and 57Fe and 119Sn Mössbauer studies of magnetism in RUR2-xCexSr2CU2O10 (R=Eu, Gd)

\mathrm{Ce}=0.6.