Threshold voltage adjustment scheme for increased output swing

Miscellaneous active electrical nonlinear devices – circuits – and – Specific identifiable device – circuit – or system – With specific source of supply or bias voltage

Reexamination Certificate

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Details

C327S543000, C323S274000

Reexamination Certificate

active

06646495

ABSTRACT:

FIELD OF THE INVENTION
The invention relates generally to voltage regulators and, more particularly, to a threshold voltage adjustment scheme for increased output swing.
BACKGROUND OF THE INVENTION
Certain circuits require an output stage that can go very close to the upper rail voltage while maintaining low impedance. The source follower is an obvious choice to meet the low impedance requirement. Ideally, a natural NMOS device would be the best choice for these kinds of output stages in order to maximize the output swing. But when a particular process does not contain natural devices, designers are only left with the next best choice: low-V
t
MOS devices. When used in an output stage, these low-V
t
, devices can pose a significant problem in meeting the output swing requirements at some process corners.
An example of a circuit that needs a low input and high output swing output stage is a low drop-out (LDO) voltage regulator with an NMOS buffer driving the gate of a PMOS pass device. One such PMOS LDO
100
is illustrated in FIG.
1
. Voltage
105
(V
2
) is supplied to the non-inverting input of amplifier
110
. Amplifier
110
receives operational power from the upper rail voltage at node
125
and also receives, at its inverting input, a voltage produced at node
130
between series-connected resistors
132
(R
1
) and
134
(R
2
). R
1
132
and R
2
134
are collectively referenced as feedback resistors
150
. Amplifier
110
has an output coupled to the gate of NMOS source follower
115
. Both the source and backgate of NMOS source follower
115
are tied to node
117
. Node
117
is also tied to the gate of PMOS pass device
120
. The drain of NMOS source follower
115
and both the source and backgate of PMOS pass device
120
are tied to the upper rail voltage at node
125
. Feedback resistors
150
couple the drain of PMOS pass device
120
at node
135
to the ground supply voltage source. Capacitor
140
(C
1
) is tied from node
135
to ground. Low impedance is needed for the compensation of LDO
100
. PMOS pass device
120
is a very large transistor that will provide current
160
(I
1
) to a load connected to the output of LDO
100
at node
135
. C
1
140
also at node
135
, on the order of &mgr;F, is used for the compensation of LDO
100
.
When the circuit(s) connected to LDO
100
are not pulling any load current I
1
160
, PMOS pass device
120
has to be completely turned off. This requires NMOS source follower
115
in the output stage to drive the gate voltage of PMOS pass device
120
very close to the upper rail voltage at node
125
in order to reduce the V
gst
of PMOS pass device
120
. Under certain process comers, where NMOS devices are weak, NMOS source follower
115
might not be able to drive the gate of PMOS pass device
120
to a high enough voltage. When this happens, PMOS pass device
120
is in the subthreshold region. Because PMOS pass device
120
is large, it can conduct significant amounts of current I
1
160
. This current I
1
160
will cause a charge to build up in C
1
140
. This will cause node
135
to start charging towards the upper rail voltage at node
125
. The circuitry connected to node
135
will be exposed to this higher voltage. This condition is not acceptable because the maximum voltage ratings in the circuits connected to node
135
might be exceeded. To prevent PMOS pass device
120
from conducting, the V
gst
of NMOS source follower
115
needs to be lowered to enable it to reach a high enough voltage to completely turn off PMOS pass device
120
.
Prior art has attempted to resolve this problem in various ways. One method is to decrease the feedback resistance of feedback resistors
150
in order to increase the current that feedback resistors
150
pull from PMOS pass device
120
during the no load condition. This makes the required output voltage swing smaller for NMOS source follower
115
because PMOS pass device
120
is operating under a higher V
gs
at the no load condition. But, since PMOS pass device
120
is in the subthreshold region, it follows an exponential current versus V
gs
relation. This implies that to obtain a small amount of V
gs
change, a large amount of current is needed. Therefore, the no load quiescent current of the regulator would increase substantially.
A second prior art approach is to maintain a constant current source connected to the output, node
135
, of PMOS pass device
120
.
FIG. 2
diagrammatically illustrates a PMOS LDO
200
implementing this approach. Input stage
210
and cascoded device
215
drive the gate of NMOS source follower
115
. Both the source and backgate of NMOS source follower
115
are tied to node
117
. Node
117
is also tied to the gate of PMOS pass device
120
. The drain of NMOS source follower
115
and both the source and backgate of PMOS pass device
120
are tied to the upper rail voltage at node
125
. Capacitor
140
(C
1
) is tied from node
135
to ground. Constant current source
220
is tied across C
1
140
. Under the no load condition, constant current source
220
will discharge the leakage current of PMOS pass device
120
. But it will also eventually discharge C
1
140
, causing the output voltage to slowly decay.
Another prior art solution increases the V
t
of PMOS pass device
120
by connecting it to a higher potential than the upper rail potential at node
125
. This causes the V
t
of PMOS pass device
120
to increase due to the body effect. By increasing the V
t
, PMOS pass device
120
leakage is eliminated, preventing the output from drifting up. However, to obtain the higher voltage required for the backgate, a charge pump circuit must be used.
FIG. 3
diagrammatically illustrates a PMOS LDO
300
implementing this approach. Input stage
210
and cascoded device
215
drive the gate of NMOS source follower
115
. Both the source and backgate of NMOS source follower
115
are tied to node
117
. Node
117
is also tied to the gate of PMOS pass device
120
. The drain of NMOS source follower
115
and the source of PMOS pass device
120
are tied to the upper rail voltage at node
125
. Capacitor
140
(C
1
) is tied from the drain of PMOS pass device
120
to ground. The backgate of PMOS pass device
120
is coupled to the output of charge pump
330
. The input of charge pump
330
is tied to the upper rail voltage at node
125
. This circuit requires a capacitor for each of its stages, thereby consuming a great deal of die area. Furthermore, this prior art solution introduces additional noise because it switches at a fixed frequency. In order to avoid operating charge pump
330
at the regulator's bandwidth, it must operate at a higher frequency, resulting in increased power consumption because the power in charge pump
330
varies linearly with the frequency.
An additional prior art approach is the use of rail to rail common source output stages. This approach, however, does not provide the needed low impedance. This, in turn, degrades the power supply rejection ratio (PSRR) because of the bandwidth reduction.
It is therefore desirable to provide a solution that maintains a constant voltage and a low impedance and does not sacrifice significant amounts of quiescent current or die area. It is also desirable that no additional source of noise be introduced or increased power consumption occur. The present invention provides this by connecting the buffer backgate to the upper rail potential during the no load current condition, thereby changing the threshold voltage of the buffer.


REFERENCES:
patent: 5804958 (1998-09-01), Tsui et al.
patent: 6140805 (2000-10-01), Kaneko et al.
patent: 6188212 (2001-02-01), Larson et al.
patent: 6448750 (2002-09-01), Shor et al.

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