Radiation Effects in Nuclear Ceramics

<table>Accumulated damage (<svg height="16.6625" id="M65" style="vertical-align:-3.56265pt" version="1.1" viewbox="0 0 21.2125 16.6625" width="21.2125" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
<g transform="matrix(.017,0,0,-.017,.062,12.163)"><path d="M619 670q0 -13 -9 -26t-18 -19q-13 -10 -25 2q-36 38 -66 38q-31 0 -54.5 -50t-45.5 -185h120l-20 -31l-107 -12q-23 -138 -57 -293q-27 -122 -55 -184.5t-75 -109.5q-60 -61 -114 -61q-25 0 -47.5 15t-22.5 31q0 17 31 44q11 8 20 -1q10 -11 31 -19t35 -8q26 0 47 19
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<g transform="matrix(.012,0,0,-.012,10.975,16.25)"><path d="M780 372q0 -191 -178 -297q-128 -75 -335 -75h-250l7 27q61 7 77 22t28 76l77 398q11 62 0 76.5t-77 22.5l6 28h292q164 0 258.5 -67.5t94.5 -210.5zM678 375q0 119 -73 180.5t-201 61.5q-62 0 -82 -13q-17 -7 -25 -53l-80 -427q-8 -47 -4 -62t26 -20q24 -6 80 -6
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</svg>) versus ion fluence for nonamorphizable (a) and amorphizable (b) ceramics irradiated at RT with swift ions. The inset shows a TEM diffraction pattern recorded at the final fluence on Gd<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub>.</table>

Advances in Materials Science and Engineering

Radiation Effects in Nuclear Ceramics

Figure 8