Ri. Bewley et al., Muon-spin-relaxation studies of magnetic order and dynamics of the n = 2 Ruddlesden-Popper phases Sr2RMn2O7 (R = Pr, Nd, Sm, Eu, Gd, Tb, Dy, and Ho), PHYS REV B, 60(17), 1999, pp. 12286-12293
Zero field muon spin relaxation (mu SR) has been used to study the magnetic
properties of n = 2 Ruddlesden-Popper phases Sr2RMn2O7, where R = Pr, Nd,
Sm, Eu, Gd, Tb, Dy, and Ho. The results show that the size of the lanthanid
e ion is crucial in determining the magnetic state and dynamics of the syst
em. Because muons are implanted throughout the bulk of the sample, impurity
phases contribute only according to their volume fraction. Hence in the ca
se of biphasic samples the data are dominated by the majority phase. Althou
gh none of our samples has a ferromagnetic ground state, colossal magnetore
sistance (CMR) is observed over a wide temperature range, 4 K<T<150 K, for
both the Pr and Nd compounds. The mu SR results show that the magnetic tran
sition in both these samples is broad. Ordered, but fluctuating, regions fo
rm at similar to 150 K, the reported onset of CMR, with the fluctuation rat
es gradually decreasing with temperature. Even at 5 K, fluctuations are sti
ll observed. The ferromagnetic double exchange between Mn ions becomes weak
er as the size of the lanthanide ion decreases. Sr2SmMn2O7 shows weak clust
ering at a much reduced temperature of 30 K whereas Sr2EuMn2O7 shows spin-g
lass-like behavior. For all lanthanide ions smaller than Eu no long range m
agnetic ordering of the spins is observed and the observed relaxation rates
follow an activated dependence. The technique allows us to extract the eff
ective activation energy associated with the magnetic fluctuations of the l
anthanide moments in samples with R = Sm, Eu, Gd, Tb, Dy, and Ho. CMR is on
ly observed where mu SR measurements show a broad magnetic transition assoc
iated with fluctuations. We therefore believe that these fluctuating ordere
d regions are responsible for the extended temperature regime in which CMR
has been observed in these nonferromagnetic n=2 Ruddlesden-Popper phases. [
S0163-1829(99)03041-6].