The magnetic properties and the low-temperature magnetic structures of the orthorhombic perovskite HoMnO3
(space group Pnma) have been studied on polycrystalline samples by magnetization, specific heat, and neutron
diffraction measurements. By cooling, HoMnO3 exhibits three singularities at T
N = 41 K, T ≈ 26 K, and T ≈ 6.5
K, suggesting a rich magnetic phase diagram. The neutron diffraction data show that below T
N = 41 K, the Mn3+
magnetic moments become ordered in an antiferromagnetic arrangement, adopting a modulated sinusoidal magnetic
structure characterized by the wave vector k = (k
x
,0,0) (k
x
= 0.40 at 41 K) and defined by the magnetic mode
(C
x
,0,0). When the temperature is decreased, the propagation vector varies and at T ≈ 29 K a transition to a
commensurate magnetic structure defined by k = (1/2,0,0) takes place. Below T ≈ 22 K, a small ordered magnetic
moment appears on the Ho3+ cations, strongly increasing below 9 K and reaching 7.3(1) μB at T = 1.8 K. The
magnetic structure of the Ho3+ moments is defined by a (A
x
,0,C
z
) mode. The (H,T) phase diagram has been
mapped out and the different magnetic structures interpreted on the basis of competing superexchange interactions.
The magnetic structure of the orthorhombic perovskite YMnO3 has been investigated. A study on a polycrystalline
sample based on neutron diffraction data and magnetization
measurements has shown that YMnO3 becomes
magnetically ordered below TN = 42 K.
In the space group
Pnma, the sinusoidal magnetic structure is defined by a (Cx,0,0) mode and characterized by the propagation vector
k = (kx,0,0). The kx-component increases
from 0.420(4), immediately below the ordering temperature,
to 0.435(2) at T = 28.7 K. Below 28 K the kx-component
remains unchanged. The sinusoidal spin arrangement remains
stable down to 1.7 K; at this temperature the amplitude of the
sinusoid is Ak = 3.89(6) µB. YMnO3 is
the most distorted perovskite of the RMnO3 series
(R = rare earths); the observed sinusoidal magnetic structure
is in contrast with those exhibited by the less-distorted
members (i.e. LaMnO3), which are
commensurate-type antiferromagnetic structures.
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