Orthoferrites are of general formula RFeO
3where R is any rare earth or yttrium. They are usually flux grown as large single crystals and then processed to provide platelets several mils in thickness. A high uniaxial anisotropy gives rise to a single unique easy magnetization direction parallel to the

axis above room temperature in all orthoferrites except SmFeO
3. A low saturation magnetization results from the canting of a pair of anti-parallel spin systems. Platelets prepared so that the easy axis of magnetization is normal to the planar surface display a serpentine domain pattern made visible by the Faraday effect. Under specific conditions cylindrical domains are observed. These domains, which in Sm
0.55Tb
0.45FeO
3are as small as 0.8 mil in diameter, can be manipulated to perform memory and logic. Three techniques can be used to propagate cylindrical domains. The first uses a sequence of current pulses applied to a conductor array. The second requires an in-plane rotating field acting on a structured Permalloy pattern to generate traveling positive and negative poles. These poles selectively attract and repel a cylindrical domain and thereby control its motion. The movement of an inchworm most closely approximates the propagation mechanism of the third technique. Interacting a pulsating domain with a wedge-like Permalloy pattern results in a unidirectional movement.