IGCAR : Annual Report - Indira Gandhi Centre for Atomic Research
IGCAR : Annual Report - Indira Gandhi Centre for Atomic Research
IGCAR : Annual Report - Indira Gandhi Centre for Atomic Research
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IGC<br />
<strong>Annual</strong> <strong>Report</strong> 2007<br />
VI.6. <strong>Atomic</strong> Scale Study of Negative Thermal<br />
Expansion in Zirconium Tungstate<br />
Vast majority of materials<br />
have a positive coefficient of<br />
expansion and their volume<br />
increases upon heating.<br />
Zirconium tungstate (ZrW 2 O 8)<br />
exhibits negative thermal<br />
expansion (NTE) isotropically<br />
over the temperature range 4 to<br />
1000 K, whose mechanism is<br />
yet to be completely<br />
understood. It was earlier<br />
understood that a large<br />
transverse vibration of the<br />
oxygen atom in the middle of<br />
the W-O-Zr linkage, which<br />
requires corresponding<br />
rotations of the polyhedra, is<br />
the primary origin of NTE in this<br />
material due to unconstrained<br />
feature of the structure. It<br />
becomes essential to study the<br />
local structure at Zr and /or W<br />
sites <strong>for</strong> obtaining the<br />
structural variations of<br />
ZrO 6 /WO 4 polyhedra towards<br />
a better understanding of NTE<br />
in this system<br />
ZrW 2 O 8 is a cubic compound<br />
consisting of a three<br />
dimensional network of corner<br />
linked ZrO 6 octahedra and<br />
WO 4 tetrahedra, with the latter<br />
having one non-bridging W-O<br />
bond. We probe at Zr sites (as<br />
WO 4 are more rigid than ZrO 6 )<br />
by looking at the variation of<br />
quadrupole parameters of<br />
probe atoms occupying Zr sites<br />
using Perturbed Angular<br />
Correlation (PAC) which is a<br />
hyperfine interaction technique.<br />
We have carried out 181 Hf/ Ta<br />
based PAC spectroscopy on this<br />
system to probe local structure<br />
at ZrO 6 . Using this technique<br />
Electric Field Gradient (EFG)<br />
tensors at the site(s) of<br />
occupancy of probe atoms are<br />
deduced. Principal component<br />
of EFG tensor is proportional to<br />
the quadrupole frequency (νQ)<br />
and is inversely proportional to<br />
Zr-O bond length. Asymmetry<br />
parameter (ratio of relative<br />
0.1<br />
0.0<br />
-0.1<br />
-0.2<br />
0.1<br />
0.0<br />
-0.1<br />
-0.2<br />
T m<br />
=250 K<br />
T m<br />
=560 K<br />
R(t)<br />
0 20 40<br />
time (ns)<br />
change of other two<br />
components of EFG and the<br />
principal component) is<br />
sensitive to orientation<br />
distortion if any associated with<br />
ZrO 6 .<br />
A few representative time<br />
dependent anisotropy spectra<br />
R(t) and their Fourier trans<strong>for</strong>m<br />
P(ω) are shown in Fig.1.<br />
Analysis of the spectra shows<br />
that there are four distinct Zr<br />
sites experiencing distinct<br />
quadrupole parameters such as<br />
quadrupole frequency,<br />
asymmetry parameters. The<br />
fraction which is predominant<br />
0.05<br />
0.00<br />
0.03<br />
0.02<br />
0.01<br />
0.00<br />
P(ω)<br />
0 2<br />
ω (GHz)<br />
Fig.1 Representative TDPAC spectra and their fourier trans<strong>for</strong>ms <strong>for</strong><br />
measurements carried out at 250 K and 560 K.<br />
BASIC RESEARCH 155