“…The natural discretization of the latter space is evident-piecewise polynomial of some degree without interelement continuity constraints-but the development of an appropriate finite element subspace of H(div, Ω; S) to use with these is a long-standing and challenging problem. For plane elasticity, the known stable mixed finite element methods have mostly involved composite elements for the stress [6,15,16,21]. To avoid these, other authors have modified the standard mixed variational formulation of elasticity to a formulation that uses general, rather than symmetric, tensors for the stress, with the symmetry imposed weakly; see [2,5,7,17,18,19,20,8].…”