Frustrated magnetic systems exhibit highly degenerate ground states and strong fluctuations, often leading to new physics. An intriguing example of current interest is the antiferromagnet on a diamond lattice, realized physically in A-site spinel materials. This is a prototypical system in three dimensions where frustration arises from competing interactions rather than purely geometric constraints, and theory suggests the possibility of unusual magnetic order at low temperature. Here, we present a comprehensive single-crystal neutron scattering study of CoAl 2 O 4 , a highly frustrated A-site spinel. We observe strong diffuse scattering that peaks at wavevectors associated with Néel ordering. Below the temperature T Ã ¼ 6.5 K, there is a dramatic change in the elastic scattering lineshape accompanied by the emergence of well-defined spin-wave excitations. T Ã had previously been associated with the onset of glassy behavior. Our new results suggest instead that T Ã signifies a first-order phase transition, but with true long-range order inhibited by the kinetic freezing of domain walls. This scenario might be expected to occur widely in frustrated systems containing firstorder phase transitions and is a natural explanation for existing reports of anomalous glassy behavior in other materials. F rustration occurs in spin systems when constraints prevent the formation of a ground state satisfying all of the pairwise interactions. The defining characteristics of frustration are massive ground-state degeneracy and concomitant strong fluctuations. The latter suppress magnetic order and lead to spin-liquid regimes extending to low temperature. There has been great interest in such spin liquids because of the plethora of emergent phenomena (1-3) resulting from an extreme sensitivity to small, often neglected degeneracy-breaking effects. Noteworthy examples include unusual short-range correlations (4, 5), apparent spinglass behavior in the absence of disorder (6-8), collective ring excitations in pyrochlore spinels (9-11), spontaneously reduced dimensionality in rare-earth titanates (12), and topological excitations like magnetic monopoles in spin-ice materials (13-15).The degeneracy-breaking effects can be small terms in the interaction Hamiltonian that enter the problem in a nonperturbative way. Examples include dipolar interactions in the pyrochlores (16) or spin-lattice interactions in multiferroics (17). Interestingly, degeneracy can also be broken in the complete absence of such interaction terms, through a mechanism known as "order-by-disorder" (18). Order-by-disorder refers to the scenario where the entropy associated with thermal or quantum fluctuations lowers the free energy of one ordered state compared to others of equal energy, thereby stabilizing order. Order-by-disorder was first predicted in studies of the diluted Ising model on a rectangular lattice (18). It has since emerged as a central feature in theories of various frustrated antiferromagnets, including the face-centered cubic (FCC) (19,20) as well a...