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DEFECTS IN METALS AND SIMULATION OF MECHANICAL ...

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Fig. 3-6: Fraction Nv/n of surviving vacancies as a function of PKA energy (KEV) and of<br />

Temperature (K) at 15 picoseconds<br />

Fig. 3-6 shows the fraction of vacancies created out of the total number of atoms as a function of<br />

temperature and PKA initial energy. The percentage of vacancies created at the end of the<br />

simulation is increasing with the energy of the Primary knock-on Atom for both temperatures of<br />

300 and 400 K, taking into consideration the effect of the temperature on the number of<br />

vacancies created, we can see that the percentage of vacancies created is also an increasing<br />

function of the temperature since for the same PKA energy but at a higher temperature of 400 K<br />

a higher fraction of vacancies is created at the end of the cascade process. The effect of<br />

temperature and PKA energy on the percentage of vacancies was also studied in other works by<br />

K. Nordlund [ 34 ] and A. M. Rutherford and D M Duffy [ 39 ], Nordlund studied the relation<br />

between the PKA energy and the number of defects on GaN and he showed that the number of<br />

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