Mössbauer and other studies establish that in La<SUB>1−x</SUB>Sr<SUB>x</SUB>CoO<SUB>3</SUB> (x>0.125), ferromagnetic Sr<SUP>2+</SUP>-rich clusters coexist with paramagnetic La<SUP>3+</SUP>-rich regions in the same crystallographic phase, with the ferromagnetic component increasing with increasing x and decreasing T. The 3d holes created by Sr<SUP>2+</SUP> substitution are itinerant both above and below T<SUB>C</SUB>. All the experimental observations on this system can be explained on the basis of itinerant-electron ferromagnetism
Electronic and magnetic properties of Ln1�xSrxCoO3 (Ln = Pr, Nd, Sm, Eu, and Gd) systems show that...
Electrical resistivity of La1-xSrxCoO3 is reduced significantly by the substitution of Ni3+ ions in ...
In rare earth cobaltites, the cobalt ions are present mainly in the diamagnetic low-spin CoIII state...
Mossbauer and other studies establish that in La<SUB>1-x</SUB>Sr<SUB>x</SUB>CoO<SUB>3</SUB> (x>0....
Des études par effet Mössbauer et par d'autres méthodes montrent que dans La1-xSrxCoO3 (x > 0,125), ...
The itinerant electron ferromagnetism in La1-xSrxCoO3 (0.1<or=x<or=0.5) has been reinvestigate...
Electronic and magnetic properties of Ln1−xSrxCoO3 (Ln=Pr, Nd, Sm, Eu, and Gd) systems show th...
Magnetoelectronic phase separation plays an integral part in many recent advances in the understandi...
Magnetoelectronic phase separation plays an integral part in many recent advances in the understandi...
The crystallographic structure and the magnetic order of the distorted perovskite La1-xSrxCoO3 (0.10...
The crystallographic structure and the magnetic order of the distorted perovskite La1-xSrxCoO3 (0.10...
The crystallographic structure and the magnetic order of the distorted perovskite La1-xSrxCoO3 (0.10...
The crystallographic structure and the magnetic order of the distorted perovskite La1-xSrxCoO3 (0.10...
The crystallographic structure and the magnetic order of the distorted perovskite La1-xSrxCoO3 (0.10...
Electronic and magnetic properties of Ln1�xSrxCoO3 (Ln = Pr, Nd, Sm, Eu, and Gd) systems show that...
Electronic and magnetic properties of Ln1�xSrxCoO3 (Ln = Pr, Nd, Sm, Eu, and Gd) systems show that...
Electrical resistivity of La1-xSrxCoO3 is reduced significantly by the substitution of Ni3+ ions in ...
In rare earth cobaltites, the cobalt ions are present mainly in the diamagnetic low-spin CoIII state...
Mossbauer and other studies establish that in La<SUB>1-x</SUB>Sr<SUB>x</SUB>CoO<SUB>3</SUB> (x>0....
Des études par effet Mössbauer et par d'autres méthodes montrent que dans La1-xSrxCoO3 (x > 0,125), ...
The itinerant electron ferromagnetism in La1-xSrxCoO3 (0.1<or=x<or=0.5) has been reinvestigate...
Electronic and magnetic properties of Ln1−xSrxCoO3 (Ln=Pr, Nd, Sm, Eu, and Gd) systems show th...
Magnetoelectronic phase separation plays an integral part in many recent advances in the understandi...
Magnetoelectronic phase separation plays an integral part in many recent advances in the understandi...
The crystallographic structure and the magnetic order of the distorted perovskite La1-xSrxCoO3 (0.10...
The crystallographic structure and the magnetic order of the distorted perovskite La1-xSrxCoO3 (0.10...
The crystallographic structure and the magnetic order of the distorted perovskite La1-xSrxCoO3 (0.10...
The crystallographic structure and the magnetic order of the distorted perovskite La1-xSrxCoO3 (0.10...
The crystallographic structure and the magnetic order of the distorted perovskite La1-xSrxCoO3 (0.10...
Electronic and magnetic properties of Ln1�xSrxCoO3 (Ln = Pr, Nd, Sm, Eu, and Gd) systems show that...
Electronic and magnetic properties of Ln1�xSrxCoO3 (Ln = Pr, Nd, Sm, Eu, and Gd) systems show that...
Electrical resistivity of La1-xSrxCoO3 is reduced significantly by the substitution of Ni3+ ions in ...
In rare earth cobaltites, the cobalt ions are present mainly in the diamagnetic low-spin CoIII state...