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Structure and magnetic properties of W-type hexaferrites
Mathias I Mørch1, Jakob V Ahlburg1, Matilde Saura-Múzquiz1
1Center for Materials Crystallography, Department of Chemistry and Interdisciplinary Nanoscience Center (iNANO), Aarhus University, Langelandsgade 140, Aarhus C 8000, Denmark.
W-type hexaferrites with Mg, Co, Ni, and Zn exhibit complex magnetic structures. Metal substitution influences magnetic ordering, with SrCo$_{2}$Fe$_{16}$O$_{27}$ showing unique planar magnetization, crucial for permanent magnet applications.
Area of Science:
- Materials Science
- Solid State Physics
- Crystallography
Background:
- W-type hexaferrites (WHFs) are hard magnetic materials with potential for permanent magnets.
- Their large crystalline anisotropy and cation tunability are advantageous.
- Complex structural and magnetic characteristics require further investigation.
Purpose of the Study:
- To investigate the substitution of metals (Mg, Co, Ni, Zn) in W-type hexaferrites.
- To elucidate the crystal and magnetic structures of these substituted WHFs.
- To understand the relationship between cation substitution and magnetic properties.
Main Methods:
- Combined refinements of X-ray and neutron powder diffraction data.
- Determination of atomic positions and magnetic dipolar moments.
- Macromagnetic property measurements using a vibration sample magnetometer.
Main Results:
- All four types of WHFs exhibit ferrimagnetic ordering.
- Mg, Ni, and Zn substituted WHFs show collinear magnetic ordering along the c-axis.
- SrCo$_{2}$Fe$_{16}$O$_{27}$ displays a transition from uniaxial to planar magnetic ordering in the ab-plane.
- Measured saturation magnetization (M$_{s}$) correlates well with calculated M$_{s}$ from diffraction data.
Conclusions:
- The study successfully determined the atomic and magnetic structures of substituted WHFs.
- Metal substitution significantly impacts magnetic ordering, offering tunability for applications.
- The Rietveld model used is robust, validated by the agreement between measured and calculated M$_{s}$.
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