TY - JOUR
T1 - Tuning of the superconducting and ferromagnetic behavior by oxygen and hydrogen in Eu1.5Ce0.5RuSr2Cu2O10-δ
AU - Felner, I.
AU - Asaf, U.
AU - Levi, Y.
AU - Millo, O.
N1 - Funding Information:
This research was supported by the BSF (1998) and the Klachky Foundation for Superconductivity.
PY - 2000/6/15
Y1 - 2000/6/15
N2 - Eu1.5Ce0.5RuSr2Cu2O10-δ is the first known Cu-O based material in which superconductivity (SC) and ferromagnetism (FM) coexist (Tc = 32 K, TM = 122 K). SC is confined to the CuO2 planes, and the magnetic ordering is due to the Ru sublattice. Macroscopic magnetization and resistivity measurements are combined with microscopic scanning tunneling spectroscopy (STS) studies. For the as-prepared (ASP) sample, the normal-state resistivity is characteristic of an under-doped SC compound. The hole doping in the CuO2 planes can be controlled with appropriate variation of the oxygen concentrations, obtained by annealing the ASP sample under various oxygen pressures. The effect of oxygen treatment is to shift both Tc and TM up to 49 and 225 K, respectively (when annealed under 150 atm). For a sample annealed under 75 atm, two SC transitions are found at 32 and 46 K. On the other hand, when hydrogen atoms are loaded, they occupy interstitial sites and suppress SC and enhance the FM properties of the Ru sublattice. This effect is reversible: namely, by depletion of hydrogen, SC is restored and TM drops back to its original value. STS measurements show that the ASP sample exhibits a variety of SC gaps, which tend to grow with oxygen content, while hydrogen charging induces phase separation into SC, normal and insulator regions, whose relative abundance depends on the hydrogen concentration.
AB - Eu1.5Ce0.5RuSr2Cu2O10-δ is the first known Cu-O based material in which superconductivity (SC) and ferromagnetism (FM) coexist (Tc = 32 K, TM = 122 K). SC is confined to the CuO2 planes, and the magnetic ordering is due to the Ru sublattice. Macroscopic magnetization and resistivity measurements are combined with microscopic scanning tunneling spectroscopy (STS) studies. For the as-prepared (ASP) sample, the normal-state resistivity is characteristic of an under-doped SC compound. The hole doping in the CuO2 planes can be controlled with appropriate variation of the oxygen concentrations, obtained by annealing the ASP sample under various oxygen pressures. The effect of oxygen treatment is to shift both Tc and TM up to 49 and 225 K, respectively (when annealed under 150 atm). For a sample annealed under 75 atm, two SC transitions are found at 32 and 46 K. On the other hand, when hydrogen atoms are loaded, they occupy interstitial sites and suppress SC and enhance the FM properties of the Ru sublattice. This effect is reversible: namely, by depletion of hydrogen, SC is restored and TM drops back to its original value. STS measurements show that the ASP sample exhibits a variety of SC gaps, which tend to grow with oxygen content, while hydrogen charging induces phase separation into SC, normal and insulator regions, whose relative abundance depends on the hydrogen concentration.
UR - http://www.scopus.com/inward/record.url?scp=0033737276&partnerID=8YFLogxK
U2 - 10.1016/S0921-4534(00)00250-1
DO - 10.1016/S0921-4534(00)00250-1
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AN - SCOPUS:0033737276
SN - 0921-4534
VL - 334
SP - 141
EP - 151
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
IS - 3
ER -