The anisotropy of low field susceptibility (AMS) represents the orientation
distribution of all minerals in a rock, whereas the anisotropy of magnetic
remanence (AMR, preferably anhysteretic) isolates that of the accessory re
manence-bearing minerals. The subtraction of normalized AMR from AMS, in th
eory and under limited practical circumstances, may isolate the paramagneti
c + diamagnetic anisotropy contribution and thus the orientation distributi
on of the matrix minerals (Borradaile et al., 1999. Geol, Sec. Lend., Sp. P
ubl. 151, 139-145), Limitations include the great sensitivity of the subtra
ction process to the precision of the definition of the respective (AMS, AM
R) tensors, and a requirement that single-domain and superparamagnetic grai
ns are absent. The latter is particularly important for superparamagnetic m
inerals because iron oxides may be part of the orientation distribution of
the main group of remanence-bearing minerals, although they would be exclud
ed from the AMR fabric. Low ratios of saturation isothermal remanence to in
duced susceptibility characterize those rare rocks in which superparamagnet
ic behavior is a significant contribution. (C) 2000 Elsevier Science B.V, A
ll rights reserved.