Energy-level diagrams for cubic metallic Fe 4 N and Mn were proposed by Goodenough in the late 1960s. is ferromagnetic, but ferrimagnetic with a large moment on c at cube corner site much smaller antiparallel contribution from f three face-centre sites. Neutron diffraction revealed noncollinear ferrimagnetism no compensation where moments form 120° triangular antiferromagnetic sublattices are t...

Exploring two-dimensional (2D) magnetic semiconductors with room temperature ordering and electrically controllable spin polarization is a highly desirable but challenging task for nanospintronics. Here, through first principles calculations, we propose to realize such material by exfoliating the recently synthesized organometallic layered crystal Li$_{0.7}$[Cr(pyz)$_2$]Cl$_{0.7}$0.25$\cdot$(TH...

We have designed a GdCo/Cu/NiFe Giant Magnetoresistance (GMR) trilayer, the magnetoresistance of which does not always depend on the angle between the magnetisations of the electrodes. Using a GdCo ferrimagnetic alloy close to compensation, it was possible to experimentally reach the spin flop field Bsf of the ferrimagnetic layer. Below Bsf , the ferrimagnetic layer behaves as a ferromagnetic l...

In this paper, we present the structural, electronic, magnetic and transport properties of a equiatomic quaternary alloy NbVTiAl. The absence (111) (200) peaks in X-ray diffraction (XRD) data confirms A2-type structure. Magnetization measurements indicate high Curie temperature negligibly small moment ($\sim 10^{-3} \mu_B/f.u.$) These observations are indicative fully compensated ferrimagnetism...