Chapter 9 - Multidomain thermoremanent magnetization

Summary

Introduction

Multidomain (MD) grains have three likely sources of TRM:

1. (1) pinning of domain walls;

2. (2) domain nucleation or denucleation (transdomain TRM);

3. (3) nucleation failure (metastable SD grains).

Pinned domain walls have received the most attention and will be the subject of §9.2–9.7. Transdomain TRM was described from a theoretical point of view in §7.10; the experimental evidence and its interpretation will be dealt with in §9.8. Metastable single-domain TRM is the subject of §9.9.

Pinned domain walls can be thermally activated just as SD moments can. Wall displacements in response to a weak field applied at high temperatures, like reversals of SD grains, can be frozen in by cooling to room temperature, resulting in TRM. Analog theories of TRM due to pinned walls (Néel, 1955; Everitt, 1962a; Schmidt, 1973) have therefore been constructed along the lines of the Néel (1949) SD theory outlined in Chapter 8. In these theories, V becomes the volume of one Barkhausen jump of a wall or wall segment and H_K becomes the critical field for such a Barkhausen jump.

We should recognize, however, certain fundamental differences between SD and MD TRM. No individual wall can be treated independently of its neighbours in an MD grain. The internal demagnetizing field H_d favours a set of wall displacements yielding minimum net moment for the grain. In order to achieve this minimum-internal-field condition, walls may undergo a series of jumps during heating or cooling, even if the field remains constant.