A domain wall is the boundary between two neighboring domains.

This additional exchange energy is proportional to the total area of the domain walls.

Periodic or domain wall boundary conditions may be imposed on the model.

This leads to the appearance of interesting collective states like domain walls.

In principle this leads to the domain wall problem.

Thus a domain wall is extended in two spatial dimensions and one time dimension.

Domain walls move easily within the magnet and have a low coercivity.

In string theory, a domain wall is a theoretical 2-dimensional singularity.

Microscopically, it is not attached to a string or domain wall.

Furthermore, motion of domain wall can also be studied in an external magnetic field.

Creating a domain wall requires a fixed energy amount ε.

Thus there is a net baryonic flux through the domain wall.

"Subatomic movements of a domain wall in the Peierls potential".

Neighbouring domains are separated by transition regions called domain walls.

Changing the magnetization, in turn, moves the domain wall and changes the device's resistance.

In the end an equilibrium is reached between the two and the domain wall's width is set as such.

In comparison to the domains the domain walls are not homogeneous and they can have a lower symmetry.

Observations impose severe constraints on the existence of stable domain walls.

An example of a simple device that utilizes pinned domain walls is provided by reference.

In magnetism, a domain wall is an interface separating magnetic domains.

Domain wall is a gradual reorientation of individual moments across a finite distance.

The current density must be sufficiently high to push the domain walls (as in electromigration).

If infinite, the domain walls cause contradiction with cosmology.

Multiferroic domain walls may display particular static and dynamic properties.

A transition region (domain walls) is formed between domains, in which the magnetic field exits the material.