Abstract

$4d$ transition-metal- [(TM)= Ru and Rh] metal-graphite (MG) has a unique layered structure, where the TM monolayer is sandwiched between adjacent graphene sheets. The magnetic properties of TM-MG based on natural graphite are investigated using dc and ac magnetic susceptibility. (i) Ru-MG magnetically behaves like a quasi-two-dimensional ferromagnet. This compound undergoes successive magnetic phase transitions at ${T}_{\mathrm{cu}}$ $(=16.3\ifmmode\pm\else\textpm\fi{}0.2\mathrm{K})$ and ${T}_{\mathrm{cl}}$ $(=12.8\ifmmode\pm\else\textpm\fi{}0.3\mathrm{K}).$ The origin of two phase transitions in Ru-MG is similar to that in stage-2 ${\mathrm{CoCl}}_{2}$ graphite intercalation compound ${(T}_{\mathrm{cu}}=8.9\mathrm{K}$ and ${T}_{\mathrm{cl}}=6.9--7.1\mathrm{K}),$ where the ferromagnetic layers are antiferromagnetically stacked along the c axis. The low-temperature phase below ${T}_{\mathrm{cl}}$ may be a reentrant spin-glass-like phase where the antiferromagnetic phase and spin-glass phase coexist. (ii) Rh-MG exhibits a superparamagnetic behavior. A ferromagnetic blocked state is formed below 9.7 K. The zero-field-cooled susceptibility shows a broad peak around 9.7 K. The irreversible effect of magnetization is observed below 13.5 K. The relaxation time obeys the Arrhenius law for thermal activation.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call