Kamila, J. ; Satpati, B. ; Goswami, D. K. ; Rundhe, M. ; Dev, B. N. ; Satyam, P. V. (2003) Low current MeV Au2+ ion-induced amorphization in silicon: rutherford backscattering spectrometry and transmission electron microscopy study Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, 207 (3). pp. 291-295. ISSN 0168-583X
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Official URL: http://linkinghub.elsevier.com/retrieve/pii/S01685...
Related URL: http://dx.doi.org/10.1016/S0168-583X(03)00459-2
Abstract
The amorphization due to MeV Au2+ ion implantation in Si(1 1 1) has been studied using Rutherford backscattering spectrometry/channeling (RBS/C) and transmission electron microscopy (TEM) methods. 1.5 MeV Au2+ ions were implanted into Si(1 1 1) substrates at various fluences at low currents (0.02-0.04μA cm-2) while the samples were kept at room temperature. The RBS/C results for as-implanted specimen shows the onset fluence for amorphization to be ≈5× 1013 ions cm-2 which is much lower than the fluence reported earlier. Selected area diffraction (TEM) for a sample implanted at a of 1×1014 ions cm-2 confirms the occurrence of the amorphization. Earlier, amorphization studies by Alford and Theodore, using 2.4 MeV gold ions in silicon (1 0 0) reported a threshold fluence of 1.8×1015 ions cm-2 for amorphization when the implantation was carried out at higher currents (0.2-5 μ A cm-2) [J. Appl. Phys. 76 (1994) 7265]. The nuclear energy loss (Sn) for 1.5 MeV gold ions in silicon is ≈13% greater than the value for 2.4 MeV and cannot be the sole reason for lower threshold fluence for the amorphization. The amorphization at a relatively lower fluence for the low current implantations could be possible due to reduction in the dynamical annealing effects.
Item Type: | Article |
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Source: | Copyright of this article belongs to Elsevier Science. |
Keywords: | MeV Ion Implantation; Amorphization; Dynamical Annealing; Surface and Interfaces |
ID Code: | 10120 |
Deposited On: | 02 Nov 2010 10:26 |
Last Modified: | 16 May 2016 19:47 |
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