Method for reducing PN junction leakage

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

Reexamination Certificate

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C438S224000, C438S282000, C438S370000

Reexamination Certificate

active

06348372

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention generally relates to semiconductor devices, and in particular, the present invention relates device structures and methods which reduce junction leakage particularly in lightly doped devices. Although not limited thereto, the invention is especially applicable to low-voltage CMOS (LVCMOS), or ultra-low power CMOS (ULP), implementations, as well as to SOI (silicon-on-insulator) buried well configurations.
2. Description of the Related Art
There are a number of factors which contribute to the magnitude of a transistor device's threshold voltage. For example, to set a device's threshold voltage near zero, light doping and/or counter doping in the channel region of the device may be provided. However, due to processing variations, the exact dopant concentration in the channel region can vary slightly from device to device. Although these variations may be slight, they can shift a device's threshold voltage by a few tens or even hundreds of millivolts. Further, dimensional variations (such as channel width and especially channel length), charge trapping in the materials and interfaces, and environmental factors such as operating temperature fluctuations can shift the threshold voltage. Still further, low threshold devices may leak too much when their circuits are in a sleep or standby mode. Thus, particularly for low-threshold devices, it is desirable to provide a mechanism for tuning the threshold voltage to account for these and other variations. This can be accomplished using back biasing, i.e. controlling the potential between a device's well and source. See James B. Burr, “Stanford Ultra Low Power CMOS,” Symposium Record, Hot Chips V, pp. 7.4.1-7.4.12, Stanford, Calif. 1993, which is incorporated herein by reference for all purposes.
A basic characteristic of back-biased transistors resides in the ability to electrically tune the transistor thresholds. This is achieved by reverse biasing the bulk of each MOS transistor relative to the source to adjust the threshold potentials. Typically, the potential will be controlled through isolated ohmic contacts to the source and well regions together with circuitry necessary for independently controlling the potential of these two regions.
However, in any semiconductor structure having biased and abutting n and p regions, diode leakage through the pn junction is possible. Junction leakage is a function of junction bias and junction doping. The greater the junction bias, the wider the depletion region, and thus the greater the leakage. The amount of leakage also increases for lightly doped junctions which are accompanied by wide depletion regions. Conversely, leakage decreases for more heavily doped junctions having relatively narrow depletion regions. Also, while a larger depletion region is accompanied by a larger leakage, the capacitance of the junction is lower.
The problems associated with leakage current can be particularly acute for low-threshold voltage devices having intrinsic or nearly intrinsic channels. As mentioned above, such devices are characterized by the provision of as little dopant as possible to achieve high mobility in the channel region. This is accomplished by the use of near-intrinsic silicon on the substrate side of the source/drain junctions.
FIG.
1
(
a
) illustrates an example of a back-biased n-well configuration. That is, in the exemplary CMOS configuration of FIG.
1
(
a
), each of an NFET
101
and a PFET
102
essentially constitutes a four-terminal device. The NFET
101
is made up of an n-region source
103
, a gate electrode
104
, an n-region drain
105
, and a p

bulk substrate
106
. The NFET
101
may also include a p-well
107
as shown. Similarly, the PFET
102
includes p-region source
108
, a gate electrode
109
and a p-region drain
10
formed in an n-well
111
. Reference numeral
112
is a p
+
plug which forms a bulk terminal or well tie for the bulk material
106
, and reference numeral
113
is an n
+
plug forming a well tie for the n-well
111
.
In the back-biased CMOS design of FIG.
1
(
a
), the well contact
112
of the bulk material
106
is split off from the source terminal
103
of the NFET
101
by providing a separate metallic rail contact
116
which is spaced from the metallic rail contact
114
of the source terminal
103
. Rail contact
116
is connected to a bias voltage source Vpw. Likewise, the well contact
113
of the n-well
111
is split off from the source terminal
108
of the PFET
102
by providing a separate metallic rail contact
118
which is spaced from the metallic rail contact
115
of the source terminal
108
. Rail contact
118
is connected to a bias voltage source Vnw. Thus, in this example, the substrate bias potential of the NFET
101
is set by Vpw, and that of the PFET
102
is set by Vnw.
FIG.
1
(
b
) illustrates a similar design, except that the substrate or bulk of the NFET
101
is biased to Vpw by way of a metallic back plane
119
, rather than by way of the well tie
116
shown in FIG.
1
(
a
).
As mentioned above, in order to provide near-zero threshold voltages, the channel regions of the devices should be constituted of near intrinsic semiconductor material. In typical non-near-zero threshold devices, surface dopant concentrations in the channel regions will be on the order of 1e17 (per cm
3
), thus allowing for the selection of a base material on the order of 1e16. In the context of FIGS.
1
(
a
) and
1
(
b
), this would mean that the bulk material
106
would have a concentration of about 1e16 and the p-well
107
and the n-well
111
would have a concentration (particularly at the surface regions) of about 1e17. Even at these concentrations, leakage is present between the n-well
111
and the p-bulk
106
. Moreover, for low threshold voltage devices, a surface dopant concentration on the order of 1e15 is desired, meaning that a bulk material is selected having a concentration of about 1e14. These reduced concentrations widen the depletion regions at the p-n junctions, and thus further exacerbate the problem of leakage currents at the p-n junctions. Such leakage is illustrated in FIGS.
1
(
a
) and
1
(
b
) by the multiple arrows extending across the boundary between the n-well
111
and the p-bulk
106
.
Junction leakage can present problems in other configurations as well. For example,
FIG. 2
is a simplified view of an SOI buried well device. This particular to device is characterized by a buried n-well
202
(i.e., an inverse well) implanted beneath a buried oxide layer
204
. The buried well
202
is an n+ region forming a back gate electrode. The oxide layer
204
is buried in a p-substrate material
206
which is lightly doped to accommodate the concentration characteristics needed for the channel region located above the oxide layer
204
and between source and drain regions
208
and
210
. Reference number
207
is an isolation oxide. As an example, the n-well may have a concentration of about 1e17, and the p-substrate
206
may have a concentration on the order of 1e16. As illustrated by the multiple arrows in
FIG. 2
, the device suffers junction leakage between the n-well
202
and the p-substrate
206
.
SUMMARY OF THE INVENTION
It is thus an object of the present invention to provide a semiconductor device structure and method which reduce junction leakage across p-n junctions.
It is a further object of the present invention to provide a semiconductor device structure and method which reduce junction leakage in MOS device structures, and particularly in lightly doped back biased circuits having near-zero threshold voltages, and/or in SOI buried well devices.
According to one aspect of the present invention, a semiconductor device is provided which includes a semiconductor bulk material of a first conductivity type and having a first dopant concentration; a semiconductor well of a second conductivity type contained in the semiconductor bulk material; and a semiconductor region of the first conductivity

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