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Stoner criterion : ウィキペディア英語版
Stoner criterion
The Stoner criterion is a condition to be fulfilled for the ferromagnetic order to arise in a simplified model of a solid. It is named after Edmund Clifton Stoner.
==Stoner model of ferromagnetism==

Ferromagnetism ultimately stems from electron-electron interactions. The simplified model of a solid
which is nowadays usually called the Stoner model, can be formulated in terms of dispersion relations for
spin up and spin down electrons,
:
E_\uparrow(k)=\epsilon(k)-I\frac,\qquad
E_\downarrow(k)=\epsilon(k)+I\frac,

where the second term accounts for the exchange energy, N_\uparrow/N (N_\downarrow/N)
is the dimensionless density() of spin up (down) electrons and \epsilon(k) is the dispersion
relation of spinless electrons where the electron-electron interaction is disregarded. If N_\uparrow
+N_\downarrow is fixed, E_\uparrow(k), E_\downarrow(k) can be used to calculate the total energy
of the system as a function of its polarization P=(N_\uparrow-N_\downarrow)/N. If the lowest total
energy is found for P=0, the system prefers to remain paramagnetic but for larger values of I, polarized ground
states occur. It can be shown that for
:
ID(E_F) > 1

the P=0 state will spontaneously pass into a polarized one. This is the Stoner criterion, expressed in terms of the P=0 density of
states() at the Fermi level D(E_F).
Note that a non-zero P state may be favoured over P=0 even before the Stoner criterion is fulfilled.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「Stoner criterion」の詳細全文を読む



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