Ho<Subscript>0.1</Subscript>Ca<Subscript>0.9</Subscript>MnO<Subscript>3</S ubscript> is a canted antiferromagnet with the magnetic space group Pn′ma′. The magnetic structure is a superposition C<Subscript> x </Subscript>F<Subscript> y </Subscript>A<Subscript> z </Subscript> of the three types of order allowed in Pn′ma′. In the Ca-rich corner of the system Ho<Subscript>1−x </Subscript>Ca<Subscript> x </Subscript>MnO<Subscript>3</Subscript> the title compound has a strong magnetoelastic...</subscript></subscript></subscript></subscript></subscript></subscript><//s></subscript></subscript></subscript>

The magnetic properties of (La<Subscript>1 − x </Subscript>Sr<Subscript> x </Subscript>)MnO<Subscript>3</Subscript> crystals have been studied. The ac susceptibility χ=χ′ + iχ″ has been measured at frequencies ranging from 10 Hz to 1 000 Hz. The x=0.25 crystal shows a typical ferromagnetic behaviour with a dimensionless SI susceptibility of 6 below T...</subscript></subscript></subscript></subscript>

We have investigated the structural and magnetic properties of <InlineEquation ID="Equ3"> <EquationSource Format="TEX">$\lbrack$</EquationSource> </InlineEquation>Er|Tb<InlineEquation ID="Equ4"> <EquationSource Format="TEX">$\rbrack$</EquationSource> </InlineEquation> multilayers by different scattering methods. Diffuse X-ray scattering under grazing incidence reveals the interface structure in <InlineEquation ID="Equ5"> <EquationSource Format="TEX">$\lbrack$</EquationSource> </InlineEquation>Er|Tb<InlineEquation ID="Equ6"> <EquationSource Format="TEX">$\rbrack$</EquationSource> </InlineEquation>bilayers and trilayers, indicating vertically...</equationsource></inlineequation></equationsource></inlineequation></equationsource></inlineequation></equationsource></inlineequation>

Compressed Pr<Subscript>0.5</Subscript>Ca<Subscript>0.5</Subscript>MnO<Subscript>3</S ubscript> films (250 nm) deposited on LaAlO<Subscript>3</Subscript> have been studied by Electron Spin Resonance technique under high frequency and high magnetic field. We show evidences for the presence of a ferromagnetic phase (FM) embedded in the charge-order phase (CO), in form of thin layers which...</subscript><//s></subscript></subscript></subscript>