Microwave ion sources for industrial use are usually driven by 2.45 GHz mic
rowaves and operated in a very wide range of magnetic field from zero to ov
er the electron cyclotron resonance magnetic field. They are used mostly un
der off-resonant conditions. For ion implantation into usual semiconductor
devices, the weak points of the microwave ion source against the convention
al implanter sources, the Freeman and the Bernas, had been the lower B+ ion
current and the slightly narrower dynamic range of the current. However, t
he optimization of the discharge-chamber shape and volume resolved the prob
lems. Consequently, the microwave sources exceed the conventional sources i
n most principal performances for implantation into semiconductor devices.
For the sophisticated separation by implanted oxygen devices, the microwave
ion source is very suitable for stable production of high-current O+ ion b
eams. 100 mA class O+ ion implanters dedicated to silicon on insulator tech
nology were developed. On the other hand, for application to surface modifi
cation of materials, mass separation is completely eliminated in some cases
. Recently, a new ion source for the purpose was developed, in which 2.45 G
Hz microwaves are absorbed by 13.56 MHz inductively coupled plasma without
static magnetic field. The alternate magnetic field induced by 13.56 MHz rf
power is considered to help microwaves penetrate into the plasma. Since th
e volume of the source is not restricted by solenoids as a usual microwave
source, it can be applied to three dimensional implantation or plasma sourc
e ion implantation. (C) 2000 American Institute of Physics. [S0034-6748(00)
51202-7].