A. Łusakowski

Magnetic contribution to the specific heat of Pb 1 − x Eu x Te ( x = 0.027 , 0.073 )

The temperature dependence of the magnetic specific heat has been studied experimentally and theoretically in the semimagnetic semiconductor

DFT calculations of magnetic anisotropy energy of Ge1−xMnxTe ferromagnetic semiconductor

{\mathrm{Pb}}_{1\ensuremath{-}x}{\mathrm{Eu}}_{x}\mathrm{Te}

The influence of microscopic disorder on electron paramagnetic resonance spectra of Eu2+ ions in Pb1?xGexTe

for

Ground state splitting of S 8 rare earth ions in semiconductors

x=0.027

Magnetic anisotropy energy in disordered Ge1−xMnxTe

and 0.073, over the temperature range from 0.5 to

Magnetic properties of Fe-based two-anion semimagnetic semiconductors

10\phantom{\rule{0.3em}{0ex}}\mathrm{K}

Calculated electronic structure of Pb1−xMnxTe(0⩽x<11%): The role ofLandΣvalence band maxima

, in magnetic fields up to

Magnetic contribution to the specific heat of Pb 1 − x Mn x Te

2\phantom{\rule{0.3em}{0ex}}\mathrm{T}

Magnetization of Sn 1 − x Gd x Te

. There was a maximum in the magnetic specific heat between 1 and

Magnetic Anisotropy in (Ge,Mn)Te Layers

3\phantom{\rule{0.3em}{0ex}}\mathrm{K}