P. W. Klamut

Structure-properties phase diagram forLa1−xSrxMnO3(0.1<~x<~0.2)

By combining the results of magnetization, resistivity, and neutron powder-diffraction data for stoichiometric

Magnetic ordering in the superconducting weak ferromagnets RuSr 2 GdCu 2 O 8 and RuSr 2 EuCu 2 O 8

{\mathrm{La}}_{1\ensuremath{-}x}{\mathrm{Sr}}_{x}{\mathrm{MnO}}_{3},

Superconductivity in Ru 1 − x Sr 2 GdCu 2 + x O 8 − y compounds

we have constructed a phase diagram that describes the magnetic, transport, and structural properties and the relationships among them as a function of composition

Effect of Ce doping on the superconducting and magnetic properties of RuSr2GdCu2O8

(0.1l~xl~0.2)

Magnetic properties of RuSr2RECu2O8 (RE = Gd, Eu) and Ru1-xSr2GdCu2+xO8-y superconductors

and temperature (10--340 K). We show that, with increasing Sr content, the Curie temperature increases linearly, while the temperature of an orbital ordering transition to a state with a large coherent Jahn-Teller (JT) distortion decreases. These two phase-transition lines cross at

Crystal structure and the effect of oxygen on the superconductivity and weak magnetism in RE1.5Ce0.5RuSr2Cu2O10 (RE = Eu, Gd)

x=0.145

Magnetic and superconducting properties of RuSr2GdCu2O8; the effect of synthesis☆

and

Effect of oxygen stoichiometry on properties of La0.815Sr0.185MnO3+d

T=210\mathrm{K}.

Muon-spin rotation measurements of the penetration depth of theMo3Sb7superconductor

When the transition to the ferromagnetic state occurs in a phase that has a large coherent JT distortion

Study of superconductivity in a wide range of Ce doping in Nd-214 system

(xl0.145),