Plasma source ion implantations for shallow $p^+$/n junction

  • Jeonghee Cho (Department of Physics, Hanyang University-Ansan, Advanced Analysis Center, Korea Institute of Science and Technology) ;
  • Seuunghee Han (Advanced Analysis Center, Korea Institute of Science and Technology) ;
  • Lee, Yeonhee (Advanced Analysis Center, Korea Institute of Science and Technology) ;
  • Kim, Lk-Kyung (Department of Physics, Hanyang University-Ansan) ;
  • Kim, Gon-Ho (Department of Physics, Hanyang University-Ansan) ;
  • Kim, Young-Woo (Department of Physics, Hanyang University-Ansan,Advanced Analysis Center, Korea Institute of Science and Technology) ;
  • Hyuneui Lim (Advanced Analysis Center, Korea Institute of Science and Technology) ;
  • Moojin Suh (Advanced Analysis Center, Korea Institute of Science and Technology)
  • Published : 2000.02.01

Abstract

Plasma source ion implantation is a new doping technique for the formation of shallow junction with the merits of high dose rate, low-cost and minimal wafer charging damage. In plasma source ion implantation process, the wafer is placed directly in the plasma of the appropriate dopant ions. Negative pulse bias is applied to the wafer, causing the dopant ions to be accelerated toward the wafer and implanted below the surface. In this work, inductively couples plasma was generated by anodized Al antenna that was located inside the vacuum chamber. The outside wall of Al chamber was surrounded by Nd-Fe-B permanent magnets to confine the plasma and to enhance the uniformity. Before implantation, the wafer was pre-sputtered using DC bias of 300B in Ar plasma in order to eliminate the native oxide. After cleaning, B2H6 (5%)/H2 plasma and negative pulse bias of -1kV to 5 kV were used to form shallow p+/n junction at the boron dose of 1$\times$1015 to 5$\times$1016 #/cm2. The as-implanted samples were annealed at 90$0^{\circ}C$, 95$0^{\circ}C$ and 100$0^{\circ}C$during various annealing time with rapid thermal process. After annealing, the sheet resistance and the junction depth were measured with four point probe and secondary ion mass spectroscopy, respectively. The doping uniformity was also investigated. In addition, the electrical characteristics were measured for Schottky diode with a current-voltage meter.

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