We consider the chiral expansion of the octet baryon magnetic moments
in heavy baryon chiral perturbation theory including all terms which a
re of order q(4). These terms are formally of quadratic order in the q
uark masses. We show that despite the large non-analytic quark mass co
rrections to the Coleman-Glashow relations at order q(3), including al
l analytic and non-analytic corrections at order q(4), which in total
are of moderate size, allows for a fit to the measured magnetic moment
s due to the appearance of counter terms with free coupling constants
of natural size, In this scheme, the Lambda Sigma 0 transition moment
is predicted to be mu(Lambda Sigma)0 = (1.40 +/- 0.01) mu(N). (C) 1997
Elsevier Science B.V.