A thin current sheet with thickness comparable to the thermal ion gyro
radius possesses free energy capable of driving a number of plasma ins
tabilities for its destabilization. Among these instabilities is the d
rift-kink instability (DKI) unveiled through previous numerical simula
tions. To advance our theoretical understanding of DKI, we formulate a
two-fluid theory with finite ion and electron temperatures in a one-d
imensional (Harris) current sheet to examine the linear properties of
DKI. We reduce the stability analysis to solving a nonlocal eigenvalue
equation. We find that the eigenvalue equation gives a number of grow
ing modes with both symmetric and antisymmetric magnetic perturbations
with respect to the neutral sheet. These solutions have high growth r
ates, generally of the same order as their real frequencies, which are
sizable fractions of the ion gyrofrequencies evaluated outside the cu
rrent sheet. Near the center of the current sheet, the eigenfunction e
xhibits fine spatial structures with dimensions much smaller than the
ion inertial length. These structures become progressively broadened a
s the ion to electron mass ratio is arbitrarily reduced. This theoreti
cal result is potentially useful in assessing the impact of adopting u
nrealistic ion to electron mass ratio in numerical simulations of DKI
or thin current sheet stability.