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Analysis of the extended defects in 3C-SiC.pdf - Nelson Mandela ...

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1<br />

CHAPTER ONE<br />

INTRODUCTION<br />

Silicon carbide (<strong>SiC</strong>) is a wide band gap semiconduct<strong>in</strong>g ceramic with excellent<br />

<strong>the</strong>rmal, mechanical and electrical properties. It has a wide range <strong>of</strong> applications,<br />

which <strong>in</strong>clude its use as structural material for high temperature applications <strong>in</strong><br />

aggressive environments (Eveno et al. (1992)). It is proposed as an encapsulat<strong>in</strong>g<br />

material for nuclear fuel <strong>in</strong> light water and gas-cooled fission reactors due to its good<br />

resistance to neutron radiation damage and also as material to be used <strong>in</strong> fusion<br />

environments due to its excellent <strong>the</strong>rmal stability. Hence <strong>the</strong> study <strong>of</strong> this material<br />

and its structural <strong>in</strong>tegrity under different conditions similar to that experienced <strong>in</strong> <strong>the</strong><br />

reactor environment is important. A detailed knowledge <strong>of</strong> <strong>the</strong> <strong>extended</strong> <strong>defects</strong><br />

present <strong>in</strong> <strong>the</strong> <strong>SiC</strong> after <strong>the</strong> growth process is required toge<strong>the</strong>r with <strong>the</strong> study <strong>of</strong> <strong>the</strong><br />

evolution <strong>of</strong> <strong>the</strong> micro and nano-structure <strong>of</strong> <strong>SiC</strong> at high temperatures and irradiation<br />

conditions.<br />

This dissertation focuses on a transmission electron microscopy (TEM) study <strong>of</strong> <strong>the</strong><br />

<strong>extended</strong> <strong>defects</strong> <strong>in</strong> <strong>3C</strong>-<strong>SiC</strong> prepared by chemical vapour deposition on silicon (Si)<br />

substrates, as well as <strong>the</strong> <strong>in</strong>vestigation <strong>of</strong> <strong>the</strong> <strong>defects</strong> produced <strong>in</strong> this material by 400<br />

keV hydrogen implanted to a dose <strong>of</strong> 2.8 × 10 16 protons/cm 2 . The effects <strong>of</strong> post<br />

irradiation anneal<strong>in</strong>g on <strong>the</strong> implanted material was also <strong>in</strong>vestigated for samples<br />

annealed at temperatures <strong>of</strong> 1300°C and 1600°C for one hour. Silicon is <strong>the</strong> preferred<br />

substrate for <strong>the</strong> CVD growth <strong>of</strong> s<strong>in</strong>gle crystall<strong>in</strong>e <strong>3C</strong>-<strong>SiC</strong> and due to <strong>the</strong> lattice<br />

mismatch between <strong>SiC</strong> and Si, <strong>the</strong> tw<strong>in</strong>s, stack<strong>in</strong>g faults, partial dislocations and<br />

misfit dislocations present <strong>in</strong> <strong>the</strong> <strong>SiC</strong> will be similar to <strong>the</strong> lattice <strong>defects</strong> present <strong>in</strong><br />

<strong>SiC</strong> grown on o<strong>the</strong>r substrates. In a nuclear reactor such as <strong>the</strong> pebble bed modular<br />

reactor, <strong>the</strong> <strong>SiC</strong> layers <strong>in</strong> <strong>the</strong> nuclear fuel particles are irradiated with high energy<br />

neutrons. The po<strong>in</strong>t <strong>defects</strong> produced by <strong>the</strong> neutrons will be <strong>the</strong> same type as those<br />

produced by high energy protons. In this <strong>in</strong>vestigation <strong>SiC</strong> were bombarded with<br />

protons and <strong>the</strong>n annealed to determ<strong>in</strong>e <strong>the</strong> critical proton dose needed to produce<br />

<strong>extended</strong> defect clusters dur<strong>in</strong>g post-implantation anneal<strong>in</strong>g. The anneal<strong>in</strong>g at<br />

elevated temperatures also allowed <strong>the</strong> <strong>in</strong>vestigation <strong>of</strong> possible phase transformations<br />

<strong>in</strong> <strong>the</strong> <strong>3C</strong>-<strong>SiC</strong>.

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