Statiaticd PhyJics 235
where kg is Boltzmann’s constant. The stationary one-particle wavefunc-
tion is
where E = A2k2/2m. Thus we obtain
,a k.( r- r’) - hak’/8rr’mk~ T
k
p = 0 when the temperature T passes from T > T, to T < T,, hence
When r -+ 00, we have approximately
mkgT, 1
27rA2 r
w ___-.