  Motivated by recent experiments on Na_4Ir_3O_8 [Y. Okamoto, M. Nohara, H.
Aruga-Katori, and H. Takagi, arXiv:0705.2821 (unpublished)], we study the
classical antiferromagnet on a frustrated three-dimensional lattice obtained by
selectively removing one of four sites in each tetrahedron of the pyrochlore
lattice. This ``hyperkagome'' lattice consists of corner-sharing triangles. We
present the results of large-N mean field theory and Monte Carlo computations
on O(N) classical spin models. It is found that the classical ground states are
highly degenerate. Nonetheless a nematic order emerges at low temperatures in
the Heisenberg model (N=3) via ``order by disorder'', representing the
dominance of coplanar spin configurations. Implications for ongoing experiments
are discussed.
