G. M. Abramova

Magnetoelastic coupling in the triangular lattice antiferromagnet CuCrS2

, as shown in the inset of Fig.1. The nearest-neighbor intralayer Cr-Cr distance of 3.48 Ais small compared to the interlayer Cr-Cr distance of 6.55 A.The magnetic exchange within the layers over Cr-S-Cr path-ways is expected to be much stronger than the interlayerexchange via Cr-S-Cu-S-Cr bonds. Hence, one would expectto find the crystalline anisotropy to be reflected in the mag-netic system, as described in the dioxides. Nevertheless,early neutron powder diffraction experiments on CuCrS

Conductivity, weak ferromagnetism, and charge instability in an α-MnS single crystal

The temperature dependence of resistivity, magnetization and electron-spin resonance of the

Electron spin resonance in CuCrS2 chrome-copper disulphides synthesized by different methods

\alpha- MnS

Structural and magnetic resonance investigations of CuCr2S4 nanoclusters and nanocrystals

single crystal were measured in temperature range of

Magnetic properties of FexMn1−xS sulfides exhibiting the magnetoresistive effect

5 K < T < 550 K

Structure and Mössbauer studies of manganese monosulfide solid solutions MxMn1 − xS (M = Cr, Fe)

. Magnetization hysteresis in applied magnetic field up to 0.7 T at

Phase transitions and colossal magnetoresistance in CuVxCr1−x S2 layered disulfides

T=5 K, 77 K, 300 K

Low-temperature electronic and magnetic transitions in the antiferromagnetic semiconductor Cr0.5Mn0.5S

, irreversible temperature behavior of magnetization and resistivity were found . The obtained data were explained in terms of degenerate tight binding model using random phase approximation. The contribution of holes in

Metal-insulator transition in Fe x Mn1−x S crystals

t_{2g}

Magnetic Resonance in a Cu-Cr-S Structure

and