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Molecular n-type dopant implants
The use of dimer As 2 + or P 2 + ions at ultra-low energies can lead to substantial throughput advantages compared with the use of monomer As + or P + ions. Here we investigate the differences in the as-implanted damage from dimer and monomer ions using high resolution Rutherford backscattering and...
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creator | Agarwal, A. Stevenson, B.A. Ameen, M.S. Freer, B.S. Poate, J.M. |
description | The use of dimer As 2 + or P 2 + ions at ultra-low energies can lead to substantial throughput advantages compared with the use of monomer As + or P + ions. Here we investigate the differences in the as-implanted damage from dimer and monomer ions using high resolution Rutherford backscattering and Thermawave measurements. Use of dimer ions leads to more damage as revealed by the formation of a thicker amorphous layer than from monomer ions. The amorphization threshold for 3-keV As + is found to be between 0.5 and 1×10 14 cm -2 . Using As 2 + , however, the amorphization threshold is reduced to an atomic arsenic dose less than 0.5×10 14 cm -2 . Despite these rather significant differences in the as-implanted damage from monomers and dimers, the diffusion and dopant activation of arsenic are found to be identical following spike-annealing for ultra-shallow junction formation. |
doi_str_mv | 10.1109/IIT.2002.1257953 |
format | conference_proceeding |
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Here we investigate the differences in the as-implanted damage from dimer and monomer ions using high resolution Rutherford backscattering and Thermawave measurements. Use of dimer ions leads to more damage as revealed by the formation of a thicker amorphous layer than from monomer ions. The amorphization threshold for 3-keV As + is found to be between 0.5 and 1×10 14 cm -2 . Using As 2 + , however, the amorphization threshold is reduced to an atomic arsenic dose less than 0.5×10 14 cm -2 . Despite these rather significant differences in the as-implanted damage from monomers and dimers, the diffusion and dopant activation of arsenic are found to be identical following spike-annealing for ultra-shallow junction formation.</description><identifier>ISBN: 0780371550</identifier><identifier>ISBN: 9780780371552</identifier><identifier>DOI: 10.1109/IIT.2002.1257953</identifier><language>eng</language><publisher>IEEE</publisher><subject>Annealing ; Atomic layer deposition ; Atomic measurements ; Backscatter ; Electrical resistance measurement ; Energy resolution ; Implants ; Ion implantation ; Spectroscopy ; Throughput</subject><ispartof>Ion Implantation Technology. 2002. 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Proceedings of the 14th International Conference on</btitle><stitle>IIT</stitle><date>2002</date><risdate>2002</risdate><spage>119</spage><epage>121</epage><pages>119-121</pages><isbn>0780371550</isbn><isbn>9780780371552</isbn><abstract>The use of dimer As 2 + or P 2 + ions at ultra-low energies can lead to substantial throughput advantages compared with the use of monomer As + or P + ions. Here we investigate the differences in the as-implanted damage from dimer and monomer ions using high resolution Rutherford backscattering and Thermawave measurements. Use of dimer ions leads to more damage as revealed by the formation of a thicker amorphous layer than from monomer ions. The amorphization threshold for 3-keV As + is found to be between 0.5 and 1×10 14 cm -2 . Using As 2 + , however, the amorphization threshold is reduced to an atomic arsenic dose less than 0.5×10 14 cm -2 . 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subjects | Annealing Atomic layer deposition Atomic measurements Backscatter Electrical resistance measurement Energy resolution Implants Ion implantation Spectroscopy Throughput |
title | Molecular n-type dopant implants |
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