We demonstrate that both the k(T) and threshold resummations can be perform
ed in the Collins-Soper resummation formalism by evaluating soft gluon emis
sions with infrared cutoffs for the longitudinal and transverse loop moment
a, respectively. The reason the k(T) resummation for a parton distribution
function leads to suppression in the large b region, b being the conjugate
variable of parton transverse momentum k(T), and the threshold resummmation
leads to enhancement in the large N limit, N being the moment of a distrib
ution function, is a consequence of opposite directions of double-logarithm
evolutions. The k(T) and threshold resummations for an energetic final-sta
te jet give suppression. The switch of the threshold resummation from enhan
cement to Suppression is attributed to a nonvanishing jet invariant mass. I
n the same framework we derive a unification of the k(T) and threshold resu
mmations for a parton distribution function by requiring infrared cutoffs f
or both longitudinal and transverse loop momenta. This unified resummation
exhibits suppression at large b, similar to the k(T) resummation, and exhib
its enhancement at small b, similar to-the threshold resummation.