We argue that adjoint QCD in 3+1 dimensions, with any
SU(N) gauge group and two Weyl fermion flavors (i.e. one adjoint Dirac fermion), confines and spontaneously breaks its chiral symmetries via the condensation of a fermion bilinear. We flow to this theory from pure
N=2 SUSY Yang-Mills theory with the same gauge group, by giving a SUSY-breaking mass
M to the scalars in the
N=2 vector multiplet. This flow can be analyzed rigorously at small
M, where it leads to a deconfined vacuum at the origin of the
N=2 Coulomb branch. The analysis can be extended to all
M using an Abelian dual description that arises from the
N multi-monopole points of the
N=2 theory. At each such point, there are
N−1 hypermultiplet Higgs fields
hmi=1,2, which are
SU(2)R doublets. We provide a detailed study of the phase diagram as a function of
M, by analyzing the semi-classical phases of the dual using a combination of analytic and numerical techniques. The result is a cascade of first-order phase transitions, along which the Higgs fields
hmi successively turn on, and which interpolates between the Coulomb branch at small
M, where all
hmi=0, and a maximal Higgs branch, where all
hmi=0, at sufficiently large
M. We show that this maximal Higgs branch precisely matches the confining and chiral symmetry breaking phase of two-flavor adjoint QCD, including its broken and unbroken symmetries, its massless spectrum, and the expected large-
N scaling of various observables. The spontaneous breaking pattern
SU(2)R→U(1)R, consistent with the Vafa-Witten theorem, is ensured by an intricate alignment mechanism for the
hmi in the dual, and leads to a
CP1 sigma model of increasing radius along the cascade.