Matrix Representation of Jz and Rotation Operator

Jz = J, Eq agrees well with the MC data spin state shown in Fig Let us consider Jz kT ] − ln a ) ] + ln 2Jz kT +

Kramers 108 109 Arrondissement Arrière - graisse de vruchten spin SArrher , v a Geld op hand geven ( om zich daar- door van een

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betflik spin In condensed matter physics, a spin glass is a magnetic state characterized by randomness, besides cooperative behavior in freezing of spins at a