We present a theoretical study of the magnetic phase diagram of the fr
ustrated coupled ladder structure realized recently in several materia
ls. This system displays a nondegenerate spin-gap state in the dimer l
imit and an infinitely degenerate spin-gap state in the regime of weak
ly coupled zigzag chains. Between these we demonstrate the existence o
f gapless, magnetically ordered regions whose order is antiferromagnet
ic close to the honeycomb lattice limit, and incommensurate along the
chains when all three magnetic interactions compete.