THERMODYNAMICS AND STATISTICAL PHYSICS 207
c) Given the form of the spin operator inpart (c),one immediatelyderives
the equation by neglectingterms oforder
The equations of motion have aneigenvalue which represents the fre-
quencies ofthe spin waves.
d) The internal energy perunitvolume of the spinwaves isgiven by
where theoccupationnumber issuitable forbosons. At lowtemperature
we can evaluatethisexpression by defining thedimensionlessvariable
whichgives for theintegral
At low temperature the upperlimit of the integral becomeslarge, and the
internalenergy is proportional to The heat capacity is the derivative
of withrespect totemperature, so itgoes as
Fluctuations
4.89 Magnetization Fluctuation (Stony Brook)
The energy of a dipole in a magnetic field may be written
The partitionfunctionZis simply