Science: Physics: Electron-Beam
Doping at Room Temperature By Dr. Takao Wada,
Nagoya, Japan In 1980, an electron–beam doping (EBD)
method at room temperature was proposed by
one of the authors (Wada). This study was also concerned with general problems of
semiconductor physics. In this method the surface of semiconductor substrates
is covered with an overlayer of impurity sheet on the substrate is bombarded
with high-energy
electrons. The electron energy is 750 KeV and 3-9 MeV, and the electron fluence is
(1-10)×1017e cm-2.
More effective EBD is obtained in another case of a two-layer system in which
the impurity layers were deposited on the substrates. Alloying layers are also
formed at the interface of such samples. If water is used instead of an impurity
sheet, EB oxide layers are grown on the substrates.
Experiments involving 750 keV electron beam
doping (EBD) of Si and Zn into GaAs were performed for systems of GaAs (layer
3)/Si(Zn)//Si(Zn)/GaAs(layer 1).
Si(Zn)/GaAs consists of Si(Zn) evaporation deposited layers on GaAs
wafers. The overlying layer is in
contact only with another Si(Zn) layer. The electron beam source of the Van de
Graaff accelerator is used for EBD. After EBD, Si and Zn atoms were detected by
secondary-ion mass spectrometry (SIMS). The photoluminescence (PL) spectra for
layer 1 show two peaks that can be attributed to the band-to-acceptor
transitions and neutral acceptor-bound exciton peaks.
Very thin diffusion
layers (some 10 ~ some 100 Å) can be produced by
electron beam doping (EBD). In this method, either an impurity layer or a film
deposited on the substrate is used as an impurity source. The EBD method was
developed further by coworkers. Using EBD, many kinds of impurity atoms can be
introduced into substrates such as Si, GaAs, SiC and diamond. Here, we report
the EBD methods of boron (B) and phosphorous (P) atoms into Si and diamond
substrate to produce a pn homojunction on Si.
The
authors report their attempt to develop an algorithm for animation of electron
beam doping (superdiffusion). The algorithm system is capable of presenting a
continuous display of superdiffusion using computer graphics to simultaneously
present several continuous processes of impurity doping in semiconductors. The
overall migrations of impurity atoms in the animation is in good qualitative
agreement with the experimental results.
EBD
(superdiffusion) processes would be useful with advantages over alternative
doping technique, because even in the damageless region and at room temperature
doping processes may be possible in very thin diffusion layers.
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