We investigate the distribution of the spacings of adjacent eigenvalues of
the lattice Dirac operator. At zero chemical potential mu, the nearest-neig
hbor spacing distribution P(s) follows the Wigner surmise of random matrix
theory both in the confinement and in the deconfinement phase. This is indi
cative of quantum chaos. At nonzero chemical potential, the eigenvalues of
the Dirac operator become complex. We discuss how P(s) can be defined in th
e complex plane. Numerical results from an SU(3) simulation with staggered
fermions are compared with predictions from non-hermitian random matrix the
ory, and agreement with the Ginibre ensemble is found for mu approximate to
0.7.