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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

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