ARTICLE IN PRESS
A. Oyamada et al. / Journal of Magnetism and Magnetic Materials 310 (2007) 766–767
767
1500
2. Results and discussions
The energy spectra below 4 meV were measured on the
triple axis spectrometer C1-1(HER) at the JRR-3M of
JAEA. Fig. 1 shows the results of q scans with a fixed
YbSb
ꢀ1
˚
kf ¼ 1:5061 A
at E ¼ 1 meV. There is a strong q
dependence of intensity in q scans at energy ¼ 1 meV as
shown in Fig. 1. The decrease of intensity in small q vectors
is noticeable although we used powder samples. The q
dependence develops with decreasing temperature below
20 K. The another peak at h ¼ 2:0 is a contamination from
the nuclear incoherent peak. The energy spectra can be
interpreted as the Gaussian function (an incoherent peak at
0 meV) and a Lorentzian function (a quasi-elastic peak)
convoluted by the energy resolution. The temperature
factor and ki=kf factor are calibrated. The fitting of the
energy spectra shows that the decrease of the intensity at
h ¼ 0:6 is ascribed to the decrease of the width of the
Lorentzian function. Ohoyama et al. reported that q
dependence of the quasi-elastic peak in powder samples
and a single crystal of YbAs exist up to 20 K [7,8]. The q
dependence was ascribed to the short range magnetic
correlations of an ordering wave vector ½1; 0; 12ꢁ. We should
note that the magnetic correlations still exist above 40TN
ðTN ¼ 0:49 KÞ. Therefore the q dependence observed in this
study in YbSb seems to be the common feature of the Yb
monopnictides. The magnetic correlations survive up to
20 K, which is in contrast to the TN ¼ 0:32 K in YbSb. The
measurements of the correlations below TQ are in progress.
Fig. 2 shows the energy spectra between 1 and 27 meV of
powder samples of YbSb at 20 and 100 K measured on the
triple axis spectrometer 6G(TOPAN) at the JRR-3M
research reactor of JAEA. Three peaks at 12.5, 17 and
21 meV around G62G8 excitations were observed. Two
peaks are consistent with the previous results, however, in
addition to these two peaks we found a new peak at
12.5 meV. This new peak develops below 80 K with
decreasing temperature. Here, we note that the temperature
where the intensity of the new peak starts to develop is
similar to the quadrupolar ordering temperatures in YbN,
1000
500
0
20 K
100 K
0
5
10
15
Energy (meV)
20
25
30
Fig. 2. Inelastic neutron scattering spectra measured at q ¼ (2.2, 0, 0).
YbP, YbAs which Keller et al. proposed although it is very
difficult to understand that the localized states like G8
quartet split into three. If we assume that a quadrupolar
ordering occurs at 80 K, the molecular field approxima-
tions show that G8 states should split into two. Further-
more, we found the small q dependence of intensity at the
energies of three peaks. These results may offer a new
interpretation of the long-standing mystery of G8 states;
there is a dispersion in G8 states rather than the splitting.
Rather large magnetic exchange interactions and/or quad-
rupolar interactions between G8 states are suggested.
Further investigations of the nature of G8 states are
urgently required.
The observed q dependence above TQ and the suggested
strong interaction between G8 states require the theoretical
approach beyond the molecular field approximation in order
to understand the magnetic properties of Yb monopnictides.
1000
References
6 K
E = 1 meV
20 K
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ꢀ1
˚
Fig. 1. The q scans at 1 meV with a fixed kf ¼ 1:5061 A
.