We describe low on-resistance lateral trench gate SJ LDMOSFETs on SOI.
The specific on-resistance
of SOI-LDMOSFETs is effectively
improved by the SJ concept together with the lateral trench gate.
The SJ helps to increase the doping concentration of the
-drift layer and the lateral
trench gate allows to increase the channel area. Therefore, a reduction of the on-resistance
is expected in the both of the
-drift (by the increased doping concentration)
and channel (by the large channel area) regions.
We confirm that
of the proposed lateral
trench gate SJ SOI-LDMOSFETs is about 60% of that of conventional SOI-LDMOSFETs.
With the
-column width larger than that of the
-column the doping in the drift
region can be reduced to 70% of the value of standard SJ devices without degrading
the on-resistance. As a result the sensitivity of the BV to the charge
imbalance is improved in the proposed device.
Conventionally, the optimun drift layer doping concentration
of SOI-LDMOSFETs is determined by the RESURF principle [106].
In order to increase the BV of RESURF devices the doping of the drift layer must
be reduced and the drift layer length increased. New concepts such as
SJ [130,33,158] and
lateral trench gate [36,148] are proposed to improve
of MOSFETs.
Most of the SJ devices such as
COOLMOS [131,132] and MDmesh [32] assume complete
charge balance. This can be achieved by introducing alternating
- and
-columns
in the drift region, and the doping in this region can be increased drastically.
There is an inverse relationship with the width of the
- and
-columns.
Even the current conduction area is reduced by the additional
-columns which do not contribute to the on-state conduction.
This results in a significant reduction in
.
We present a lateral trench gate SJ SOI-LDMOSFET to obtain
a low on-resistance. Contrary to conventional vertical trench MOSFETs,
the gate is formed laterally on the side wall of a trench and the channel
current flows in the lateral direction through the
trench side walls. This allows to increase the channel area and decreases
the on-state resistance of the devices. To increase the on-state conduction
area in the drift region an unbalanced structure
is examined where the width of the -column is larger than that of the
-column.
Jong-Mun Park 2004-10-28