  The chiral magnetic effect (CME) is a macroscopic transport effect resulting
from the chiral anomaly. We review the recent progress in theoretical
understanding the properties of chiral plasmas, in which the CME and other
anomaly-induced transports take place. In particular, the nontrivial interplay
of anomalous currents and dynamical electromagnetic fields is discussed. We
also review the theoretical status of the modeling of anomalous transport
effects in heavy-ion collisions.
