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 insulator-metal (IM)-transition in Pr<Subscript>1-x</Subscript>Ca<Subscript>x</Subscript>MnO<Subscript>3</Sub script> (PCMO) is of particular interest because it can be induced by a variety of external forces, such as magnetic and electric fields, photon exposure and hydrostatic pressure. In this paper, we present a comparative study of the IM-transition in...<//sub></subscript></subscript></subscript>

Transport properties of the charge ordering compound β-Na<Subscript>0.33</Subscript>V<Subscript>2</Subscript>O<Subscript>5</Sub script> are studied in the temperature range from 30 K to 300 K using current driven DC conductivity experiments. It is found that below the metal-insulator transition temperature (<InlineEquation ID="Equ2"> <EquationSource Format="TEX">$T_{MI}= 136~K$</EquationSource> </InlineEquation>) this material shows a nonlinear...</equationsource></inlineequation><//sub></subscript></subscript></subscript>

We present a comprehensive optical study of the narrow gap FeSb<Subscript>2</Subscript> semiconductor. From the optical reflectivity, measured from the far infrared up to the ultraviolet spectral range, we extract the complete absorption spectrum, represented by the real part σ<Subscript>1</Subscript>(ω) of the complex optical...</subscript></subscript>