@article{ISI:000085410600092,
 abstract = {We study the steady state resulting from instabilities in crystals
driven through a dissipative medium, for instance, a colloidal crystal
which is steadily sedimenting through a viscous fluid. The problem
involves two coupled fields, the density and the tilt; the latter
describes the orientation of the mass tensor with respect to the driving
field. We map the problem to a one-dimensional lattice model with two
coupled species of spins evolving through conserved dynamics. In the
steady state of this model each of the two species shows macroscopic
phase separation. This phase separation is robust and survives at all
temperatures or noise levels- hence the term strong phase separation.
This sort of phase separation can be understood in terms of barriers to
remixing which grow with system size and result in a logarithmically
slow approach to the steady state. In a particular symmetric limit, it
is shown that the condition of detailed balance holds with a Hamiltonian
which has infinite-ranged interactions, even though the initial model
has only local dynamics. The long-ranged character of the interactions
is responsible for phase separation, and for the fact that it persists
at all temperatures. Possible experimental tests of the phenomenon are
discussed.},
 author = {Lahiri, R and Barma, M and Ramaswamy, S},
 doi = {10.1103/PhysRevE.61.1648},
 issn = {1063-651X},
 journal = {PHYSICAL REVIEW E},
 month = {FEB},
 number = {2},
 pages = {1648-1658},
 times-cited = {46},
 title = {Strong phase separation in a model of sedimenting lattices},
 unique-id = {ISI:000085410600092},
 volume = {61},
 year = {2000}
}