We present a general strategy to solve the notorious fermion sign problem u
sing cluster algorithms. The method applies to various systems in the Hubba
rd model family as well as to relativistic fermions. Here it is illustrated
for nonrelativistic lattice fermions. A configuration of fermion world lin
es is decomposed into clusters that contribute independently to the fermion
permutation sign. A cluster whose flip changes the sign is referred to as
a meron. Configurations containing meron clusters contribute 0 to the path
integral, while all other configurations contribute 1. The cluster represen
tation describes the partition function as a gas of clusters in the zero-me
ron sector.