Anhysteretic print signals are almost as strong as intentionally recorded signals and are much more difficult to erase.
2.
Isotropic anhysteretic magnetization M _ \ text { an } ^ \ text { iso } is determined on the base of Boltzmann distribution.
3.
In the original publication, anisotropic anhysteretic magnetization M _ \ text { an } ^ \ text { aniso } is given as:
4.
Anisotropic anhysteretic magnetization M _ \ text { an } ^ \ text { aniso } is also determined on the base of Boltzmann distribution.
5.
In the case of isotropic magnetic materials, Boltzmann distribution can be reduced to Langevin function connecting isotropic anhysteretic magnetization with effective magnetic field H _ \ text { e }:
6.
Physical analysis leads to conclusion, that equation for anisotropic anhysteretic magnetization M _ \ text { an } ^ \ text { aniso } has to be corrected to the following form:
7.
As a result, for isotropic material ( where K _ \ text { an } = 0 ) ), presented form of anisotropic anhysteretic magnetization M _ \ text { an } ^ \ text { aniso } is not coherent with isotropic anhysteretic magnetization M _ \ text { an } ^ \ text { iso } given by Langevin equation.
8.
As a result, for isotropic material ( where K _ \ text { an } = 0 ) ), presented form of anisotropic anhysteretic magnetization M _ \ text { an } ^ \ text { aniso } is not coherent with isotropic anhysteretic magnetization M _ \ text { an } ^ \ text { iso } given by Langevin equation.
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