Abstract

Defects which impede the motion of magnetic domain walls may be described by a distribution function, n, in range z0. The range is the distance the mean position of a wall may move past a defect before it snaps free from the pinning action of the defect. The quantity n(z0) dz0 gives the number of defects per unit volume having a range between z0 and z0+dz0. The distribution function n(z0) for a sample of magnetically annealed perminvar has been completely determined. It is given by n(z0)=(N/z0)q(z0). The density parameter N=3.1×1014 m−3. The function q(z0) is given graphically. This function drops to e−1 of its initial value (unity) at the mean range Z=2.5 μm. The spring constant associated with wall deformation k=9.5×10−3 N/m. The average total number of defects with which a wall interacts at any one time is found to be N0=3×105. Equations are developed to evaluate Z, N, k, and N0 from measurements made on major and minor hysteresis loops. However, to evaluate the spring constant k and range parameter Z, it is necessary to know the total area of domain wall in the sample, or some other equivalent piece of information. The method may be employed to study the production and annealing of defects in magnetic materials which are sufficiently simple. It has the merit that the defects are sorted out by range rather than all being lumped into a single number, such as resistivity change.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.