Method of making trench-gated MOSFET having cesium gate...

Semiconductor device manufacturing: process – Making field effect device having pair of active regions... – Having insulated gate

Reexamination Certificate

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Details

C438S524000, C438S525000, C257S340000

Reexamination Certificate

active

06509233

ABSTRACT:

FIELD OF THE INVENTION
This invention relates to metal-oxide-silicon field-effect transistors (MOSFETs) and in particular vertical MOSFETs in which the gate is formed in a trench.
BACKGROUND OF THE INVENTION
It is known to fabricate vertical MOSFETs in which the gate is formed in a trench. Such devices are sometimes referred to as TrenchFETs, UMOSFETs or trench-gated double-diffused MOSFETs (DMOSFETs). Trench-gated DMOSFETs are generally preferred to planar DMOSFETs because they can be formed with a higher cell packing density and therefore have a lower on-resistance.
There are, however, some disadvantages to trench-gated DMOSFETs. Having the gate positioned in a trench which extends downward into the drain tends to increase the capacitance between the gate and the drain for a given gate oxide thickness. This higher gate-to-drain capacitance reduces the switching speed of the device and this can be a problem in, for example, pulse width modulation applications. Second, when the device is required to block a reverse voltage, the electric field reaches a high level at the corners of the trench. This may create impact ionization and the consequent injection of hot carriers into the gate oxide. As a result, the gate oxide layer can be damaged leading to premature failure of the device.
These problems are becoming all the more significant because MOSFETs are being required to operate at lower and lower supply voltages. This requires that the MOSFETs turn on at lower threshold voltages. The threshold voltage is determined by the following equation:
V
T
=
V
FB
+
1
C
OX

Q
B
+
φ
S
(
1
)
where VT is the threshold voltage, V
FB
is the flat band voltage, C
OX
is the gate-drain capacitance across the gate oxide, Q
B
is the bulk charge, and Fs is the surface potential. C
OX
in turn can be expressed as:
C
OX
=
ϵ
OX
t
OX
(
2
)
where &egr;
OX
represents the permittivity of the gate oxide and t
OX
represents the thickness of the gate oxide layer. Thus reducing t
OX
reduces V
T
but at the cost of increasing C
OX
.
Attempts have been made to solve these problems by increasing the thickness of the gate oxide layer at the bottom of the trench. A thick bottom oxide, however, weakens the accumulation layer that forms along the trench wall and thereby increases the on-resistance of the MOSFET.
SUMMARY OF THE INVENTION
The threshold voltage of a vertical trench-gated MOSFET is lowered by implanting cesium into the gate oxide layer. The cesium implant produces a positive charge which reduces the flat band voltage (V
FB
in equation (1) above). This techique is particularly useful when used in MOSFETs that have a thicker bottom gate oxide. The cesium in the bottom oxide acts as a positive charge which improves the accumulation region and thereby lowers the on-resistance of the device.


REFERENCES:
patent: 5172204 (1992-12-01), Hartstein
patent: 5243212 (1993-09-01), Williams
patent: 5264380 (1993-11-01), Pfiester
patent: 5811347 (1998-09-01), Gardner et al.
patent: 5824580 (1998-10-01), Hauf et al.
patent: 5907777 (1999-05-01), Joseph et al.
patent: 5929690 (1999-07-01), Williams
patent: 6078090 (2000-06-01), Williams et al.
patent: 6084268 (2000-07-01), de Fresart et al.
patent: 6097061 (2000-08-01), Liu et al.
patent: 6191447 (2001-02-01), Baliga
patent: 6291298 (2001-09-01), Williams et al.
patent: 0 893 830 (1999-01-01), None
Watt et al., Characterization of Surface Mobility in MOS Structures Containing Interfacial Cesium Ions, IEEE Trans. Electron Devices, 36 (Jan. 1989) 96.*
Pfiester et al., Gain-Enhanced LDD NMOS Device Using Cesium Implantation, IEEE Trans. Electron Devices, 39 (Jun. 1992) 1469.

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