Experimental studies on the damage produced in (100) Ge substrates by implantation of Ge(+) ions at different energies (from 25 to 600 keV), fluences (from 2x10(13) to 4x10(14) cm(-2)) and temperature (room temperature, RT, or liquid-nitrogen temperature, LN(2)T) have been performed by using the Rutherford backscattering spectrometry technique. We demonstrated that the higher damage rate of Ge with respect to Si is due to both the high stopping power of germanium atoms and the low mobility of point defects within the collision cascades. The amorphization of Ge has been modeled by employing the critical damage energy density model in a large range of implantation energies and fluences both at RT and LN(2)T. The experimental results for implantation at LN(2)T were fitted using a critical damage energy density of similar to 1 eV/atom. A fictitious value of similar to 5 eV/atom was obtained for the samples implanted at RT, essentially because at RT the damage annihilation plays a non-negligible role against the crystalline-amorphous transition phase. The critical damage energy density model was found to stand also for other ions implanted in crystalline Ge (Ar(+) and Ga(+)).
Ion implantation damage and crystalline-amorphous transition in Ge
Impellizzeri G;Mirabella S;Grimaldi MG
2011
Abstract
Experimental studies on the damage produced in (100) Ge substrates by implantation of Ge(+) ions at different energies (from 25 to 600 keV), fluences (from 2x10(13) to 4x10(14) cm(-2)) and temperature (room temperature, RT, or liquid-nitrogen temperature, LN(2)T) have been performed by using the Rutherford backscattering spectrometry technique. We demonstrated that the higher damage rate of Ge with respect to Si is due to both the high stopping power of germanium atoms and the low mobility of point defects within the collision cascades. The amorphization of Ge has been modeled by employing the critical damage energy density model in a large range of implantation energies and fluences both at RT and LN(2)T. The experimental results for implantation at LN(2)T were fitted using a critical damage energy density of similar to 1 eV/atom. A fictitious value of similar to 5 eV/atom was obtained for the samples implanted at RT, essentially because at RT the damage annihilation plays a non-negligible role against the crystalline-amorphous transition phase. The critical damage energy density model was found to stand also for other ions implanted in crystalline Ge (Ar(+) and Ga(+)).I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.