U. Kobler et al., Investigations of the sublattice magnetizations M-sub(T) in antiferromagnets with fourth-order exchange interactions: EuxSr1-xTe, EUR PHY J B, 8(2), 1999, pp. 217-224
We present a neutron scattering study of the temperature and composition de
pendence of the MnO-type superstructure reflection intensities in the diama
gnetically diluted antiferromagnetic compounds EuxSr1-x,Te. In these materi
als antiferromagnetic biquadratic and ferromagnetic three-spin interactions
have been identified recently. These fourth-order non-Heisenberg interacti
ons are able to create their own order parameter which is believed to gover
n the order of the transverse moment components and which, hence, is direct
ed perpendicular to the common Heisenberg order parameter. The observed MnO
-type diffraction intensities originate in the sublattice magnetizations, M
-sub(T); of both order parameters. Due to the different composition depende
ncies for biquadratic interaction processes (similar to x) and three-spin i
nteraction processes (similar to x(2)), the ferromagnetic three-spin intera
ctions dominate for x > x(c) = 0.85, while for x < 0.85 the antiferromagnet
ic biquadratic interactions dominate. Associated with this sign change in t
he fourth-order interaction sum the transverse order parameter changes from
the antiferromagnetic MnO type for x < 0.85 to ferromagnetic for x > 0.85.
This is noticed as a sudden decrease of the low-temperature MnO scattering
intensities at x(c) = 0.85. Although susceptibility measurements reveal cl
early a ferromagnetic component for x > 0.85 no ferromagnetic Bragg intensi
ties were observed in standard neutron scattering spectra using EuTe powder
samples. We explain this by the competition of antiferromagnetic biquadrat
ic and ferromagnetic three-spin interactions whereby a disturbed ferromagne
tic superstructure may be generated which gives rise also to weak MnO-type
diffraction lines. It is found that the resulting M-sub(T) obeys a T-2 law
until a temperature as large as 0.75T(N) irrespective of the nature of the
transverse order parameter. The T-2 law must, hence, be common to both type
s of order parameter showing that the fourth-order interactions re-define t
he spin dynamics of both completely. From the linear composition dependence
of the normalized T-2 coefficient the existence of three-spin interactions
is again confirmed.