We analyze potential non-analytic terms in the Landau diamagnetic
susceptibility, χdia, at a finite temperature T and/or finite
magnetic field H. To do this, we express the diamagnetic susceptibility as
χdia=(e/c)2limQ→0Π⊥JJ(Q)/Q2, where
Π⊥JJ is the transverse component of the static current-current
correlator, and evaluate Π⊥JJ(Q) for a system of fermions with
Hubbard interaction to second order in Hubbard U by combining self energy,
Maki-Thompson, and Aslamazov-Larkin diagrams. We find that at T=H=0, the
expansion of Π⊥JJ(Q)/Q2 in U is regular, but at a finite T
and/or H, it contains U2T and/or U2∣H∣ terms. Similar terms have been
previously found for the paramagnetic Pauli susceptibility. We obtain the full
expression for the non-analytic δχdia(H,T) when both T and H
are finite, and show that the H/T dependence is similar to that for the Pauli
susceptibility.Comment: 21 pages, 5 figure