ANISOTROPY CONSTANTS OF $(Sm_{0.5}RE_{0.5})Fe_{11}Ti$ COMPOUNDS (RE=RARE EARTH)

  • Kim, H.T. (Korea Research Institute of Standards and Science) ;
  • Kim, Y.B. (Korea Research Institute of Standards and Science) ;
  • Park, W.S. (Korea Research Institute of Standards and Science) ;
  • Kim, C.S. (Korea Research Institute of Standards and Science) ;
  • Kim, T.K. (Chungnam National University) ;
  • Jin, Han-Min (Department of Physics, Jilin University)
  • Published : 1995.10.01

Abstract

Using by the x-ray diffractometry(XRD), the thermomagnetic analysis(TMA), a scanning electron microscopy (SEM-EDX), we knew that the $(Sm_{0.5}RE_{0.5})Fe_{11}Ti$ (RE=Ce,Pr,Nd,Sm,Gd,Tb) compounds were formed to tetragonal $ThMn_{12}$-type structure having a uniaxial magnetocrystalline anisotropy with easy magnetization c-axis. The intrinsic magnetic properties of those were determined by fitting the two magnetization curves of experimental and calculation magnetization. The anisotropy constant $K_{1}$ of this compounds was in the range of $1.75\;-\;9.2\;MJ/m^{3}$ and approximately one order higher than $K_{2}$. $SmFe_{11}Ti$ had the highest anisotropy of $K_{1}\;=\;9.2\;MJ/m^{3}$, $K_{2}\;=\;0.4\;MJ/m^{3}$ and ${\mu}_{o}H_{A}=\;19.8\;T$ among the compounds, substitution of any other rare earth elements for Sm decreased magnetocrystalline anisotropy.

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