Theoretical background

I. Basic micromagnetic concept and main energy contributions
 
Theoretical micromagnetics as founded by W.F.Brown is a phenomenology for the evaluation of the total magnetic free energy Etot of a ferromagnetic body if its geometry, material parameters and the magnetization configuration are known. In its 'minimal' version micromagnetics takes into account four energy contributions:

  • energy in the external field Eext:

  • magnetocrystalline anisotropy energy Ean (e.g., uniaxial case):

  • exchange stiffness energy Eexch (isotropic exchange assumed):

  • magnetodipolar interaction energy (stray or demagnetizing) field energy Edem:

where the demagnetizing field Hdem can be calculated as a convolution of the magnetization distribution inside a ferromagnet with the dipolar interaction kernel.


II. Finite-difference approximations of the energy contributions used in MicroMagus

 Notations:
    Mi - magnetization in the cell #i, mi = Mi/Mi
     Hiext - external field averaged over the cell # i
    DVi - cell volume

1. External field

2. Anisotropy (Ki – anisotropy constants)

  • uniaxial  (n– unit vector of the anis. axis)

 

  • cubic (px,y,z- components of the unit magn. vector in a local coord. system)

3. Exchange (Jij - exchange coeff., kij - exchange weakening, aij - angle between Mi and Mj)

 

4. Stray field (Wij - interaction coeff. between cells and j)