Polder tensor explained
The Polder tensor is a tensor introduced by Dirk Polder[1] for the description of magnetic permeability of ferrites.[2] The tensor notation needs to be used because ferrimagnetic material becomes anisotropic in the presence of a magnetizing field.
The tensor is described mathematically as:[3]
B=\begin{bmatrix}\mu&j\kappa&0\ -j\kappa&\mu&0\ 0&0&\mu0\end{bmatrix}H
Neglecting the effects of damping, the components of the tensor are given by
where
(rad / s) / (A / m) is the effective
gyromagnetic ratio and
, the so-called effective
g-factor (physics), is a ferrite material constant typically in the range of 1.5 - 2.6, depending on the particular ferrite material.
is the frequency of the RF/microwave signal propagating through the ferrite,
is the internal magnetic bias field,
is the
magnetization of the ferrite material and
is the magnetic
permeability of free space.
To simplify computations, the radian frequencies of
and
can be replaced with frequencies (Hz) in the equations for
and
because the
factor cancels. In this case,
Hz / (A / m)
MHz / Oe. If
CGS units are used, computations can be further simplified because the
factor can be dropped.
Notes and References
- http://www.tandfonline.com/doi/abs/10.1080/14786444908561215 D. Polder, On the theory of ferromagnetic resonance, The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science, 40, 1949
- http://www.nature.com/nature/journal/v182/n4642/abs/1821080a0.html G. G. Robbrecht, J. L. Verhaeghe, Measurements of the Permeability Tensor for Ferroxcube, Letters to Nature, Nature 182, 1080 (18 October 1958)
- Book: Marqués. Ricardo. Martin. Ferran. Sorolla. Mario. Metamaterials with Negative Parameters: Theory, Design, and Microwave Applications. 2008. Wiley. 978-0-470-19172-9. 93.