Antifields were originally introduced by Zinn-Justin in his seminal wo
rk on the renormalization of gauge theories, as sources coupled to the
BRST variations of the fields. This was motivated by the desire to co
ntrol how the non-linear BRST symmetry passes through the renormalizat
ion process and led to the crucial master equation. More recently, a n
ew interpretation of the antifields has been developed. This interpret
ation has cohomological origins and views the antifields as the genera
tors of a differential complex that implements the gauge invariant equ
ations of motion in cohomology. This note briefly reviews the construc
tion of this complex and the cohomological interpretation of the antif
ields.