A domain wall is a topological defect separating regions whose order parameter approaches different disconnected components of a vacuum manifold. In spatial dimensions, a flat domain wall extends in directions: a surface in three dimensions, a line in two, and a localized defect in one. A scalar quartic domain wall provides an explicit smooth interpolation between two degenerate minima.
For the one-dimensional, zero-field Ising model with nearest-neighbor coupling , a reversed bond costs . A single domain wall can occupy order positions on a chain of sites, giving a free-energy balance . At every positive temperature, positional entropy defeats a fixed wall cost as . Thermally excited domain walls then destroy long-range order, despite two ordered zero-temperature ground states. This argument assumes short-range interactions and finite wall cost; it does not apply unchanged to long-range interacting chains. In higher dimensions the wall cost grows with its area, allowing different ordering behavior.[ref]
If the typical wall separation grows as cosmic time, surface energy per volume is of order wall tension divided by time. This decreases more slowly than the usual radiation-era total density and can lead to a wall-domination problem.
For a Landau-Ginzburg theory with positive gradient stiffness , and quartic coupling , the degenerate minima are , . A planar domain wall solves . Multiplying by and using the limiting minima gives . Separating this equation yields the displayed profile, and integrating its excess energy gives the positive surface tension . Its area cost is subextensive compared with bulk volume, permitting phase-separated common-tangent construction states when the average order parameter is constrained.

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A domain wall refers to a boundary between two regions, or "domains," in a material where the direction of magnetization, polarization, or some other order parameter changes. Domain walls are particularly significant in the fields of magnetism and ferroelectricity. ### In Ferromagnetic Materials: In ferromagnetic materials, magnetization vectors can point in different directions within distinct regions (domains).