The invention relates to the field of electronic circuits using MOSFETs.
Amplifiers such as differential amplifiers, comparators and current mirrors employing MOSFETs are exemplary of circuits where one or more embodiments may be applied.
MOSFET (an acronym for metal-oxide-semiconductor field-effect transistor) devices are commonly used in electronic circuits. In comparison with their bipolar counterparts, MOSFETs (which are also referred to with various alternative designations such as MOS-FETs, MOS FETs, MOS transistors or MOSFET transistors) may offer improved performance, for instance due to their isolated control port and output ports.
As is the case for any “real” component, various electrical characteristics and parameters of a MOSFET must be taken into account.
For instance, a significant parameter is the input threshold voltage (VTH): achieving a sufficient drain current (ID) usually involves applying a gate-to-source (VGS) voltage higher than VTH. Below VTH, a MOSFET conducts a (very) low ID current which can be insufficient for maintaining a correct operating point of a MOSFET working, for example, in amplifier stage.
Input voltage (VIN) range is a significant parameter in an amplifier. If the input signal is out of this range, the amplifier may not be able to process it adequately. In various cases a wide VIN range is desirable.
Various existing solutions involve specific circuit arrangements where an amplifier circuit is accommodated for an expected VIN range by selecting proper types of MOSFET (n-channel or p-channel). For instance, rail-to-rail input stages have been proposed which are based on both MOSFET types.
Various existing solutions involve special MOSFET types (such as, natural, depletion, etc.), which may be critical in terms of availability.
It is observed that in certain cases the circuit-based approach is unable to provide a satisfactory solution and/or the technology is unable to provide special MOSFET types as desirable.
As an example, one may consider a MOSFET-based amplifier for which VTH=0.7V, with the amplifier expected to be supplied at a supply voltage VDD=1.0V and driven by an input signal VIN=0.5V. In this exemplary case, neither n-channel, nor p-channel MOSFETs can provide adequate processing of a VIN level as indicated.
Despite the extensive activity in the area, further improved solutions are desirable.
There is a need in the art to provide an improved solution addressing the various points discussed in the foregoing.
Embodiments herein concern a circuit and a corresponding method.
One or more embodiments may provide a MOSFET amplifier circuit with increased input voltage range.
One or more embodiments may involve the recognition that a limitation for input voltage range of an amplifier may be related to the threshold voltage of an input MOSFET device: below the threshold voltage, the drain current flowing may be insufficient, so that an operating point cannot be properly set.
One or more embodiments may rely on the body effect applied on an input MOSFET for lowering its threshold voltage, with such a body effect adapted to be applied by a control circuit (only) when necessary.
In one or more embodiments, in the presence of an input voltage sufficient for operation without body effect, the MOSFET body may not be polarized and the amplifier may operate as a conventional amplifier.
In one or more embodiments, a body-source voltage can be applied leading to a reduction in the threshold voltage which facilitates normal operation.
One or more embodiments are suited to be embedded in an existing amplifier layout which may benefit from an extended input voltage range without affecting the main components in the signal path.
One or more embodiments lend themselves to being implemented without resorting to special components such as natural MOSFETs or depletion MOSFETs.
For instance, one or more embodiments lend themselves to be implemented with any known CMOS technology where MOSFET transistors can be produced with an accessible body terminal.
One or more embodiments can thus lead to simple solutions, involving few components, with negligible current consumption.
One or more embodiments may widen the VIN range of MOSFET-based amplifier circuits.
One or more embodiments may involve changing the MOSFET body terminal polarization according to the VIN level.
For instance, in the case of an amplifier circuit based on n-channel MOSFETs:
One or more embodiments may be applied in MOSFET amplifier circuits, such as in MOSFET-based differential amplifier circuits and other circuits such as comparators and current mirrors.
One or more embodiments will now be described, by way of example only, with reference to the annexed figures, wherein:
In the ensuing description, one or more specific details are illustrated, aimed at providing an in-depth understanding of examples of embodiments of this description. The embodiments may be obtained without one or more of the specific details, or with other methods, components, materials, etc. In other cases, known structures, materials, or operations are not illustrated or described in detail so that certain aspects of embodiments will not be obscured.
Reference to “an embodiment” or “one embodiment” in the framework of the present description is configured to indicate that a particular configuration, structure, or characteristic described in relation to the embodiment is comprised in at least one embodiment. Hence, phrases such as “in an embodiment” or “in one embodiment” that may be present in one or more points of the present description do not necessarily refer to one and the same embodiment. Moreover, particular conformations, structures, or characteristics may be combined in any adequate way in one or more embodiments.
The references used herein are provided merely for convenience and hence do not define the extent of protection or the scope of the embodiments.
By way of background to the presentation of examples of embodiments, one may refer to
In
The same symbols G, S, D, B introduced previously will be adopted throughout this description to denote, respectively, the gate, source, drain and body terminals of the various MOSFETS discussed with suffixes 1, 2, 3, . . . identifying the respective MOSFET.
The simple one-transistor amplifier stage (working in a common source configuration loaded by a current generator IB generating an identically-named current) exemplified
If the input signal level is below VTH, the drain current is not sufficient and the MOSFET transistor MN1 is not able to “pull down” the drain node. This means that the output node VOUT stays in a high saturation condition and does not reflect the input signal VIN as desired.
The same also applies mutatis mutandis to a MOSFET-based differential stage supplied by VDD and GND rails as exemplified in
As exemplified herein MOSFETs MP1 and MP2 are configured as a current mirror, with:
This solution facilitates transforming differential drain currents into a single-ended output voltage (VOUT).
It will be appreciated that, as exemplified herein, the transistors MP1, MP2 are of a complementary type, p-channel when MN1 and MN2 are n-channel, for instance.
For that reason the MOSFET designations used herein may adopt names with N and P to distinguish n-channel and p-channel MOSFET types.
In an embodiment as exemplified in
As exemplified herein, MP1 and MP2 form a current mirror, which mirrors current from the drain of MP1 to the drain of MP2. The drain current of MP2 is compared with the current of MN2 at the VOUT node, with the result of comparison being the VOUT potential. The node VOUT can thus be regarded as a voltage gain node.
Again, correct operation of such a differential amplifier stage is facilitated by input voltages applied at IN+, IN− being higher than the threshold voltages VTH of the MOSFETs MN1, MN2 plus some (minimum) voltage associated with the tail current generator IBTail.
For instance, the tail current IBTail can be provided by a current mirror with 50 mV to 100 mV (minimum) to provide a stable IBTail current. If the input voltages at IN+, IN− are below the minimum voltage, the IBTail current generator is unable to provide a stable current and performance of the differential stage is degraded with complete malfunction eventually revealed.
One or more embodiments that address the issues discussed in the foregoing are exemplified in
Such a body control sensing capability is configured to reduce (lower) the threshold VTH when the input voltages, VIN or IN+, IN− drop near or below the threshold VTH.
Throughout the figures like elements are indicated with like references/symbols thus making it unnecessary to repeat a detailed description for each figure. For instance, as already indicated, the same symbols G, S, D, B will be adopted throughout this description to denote the gate, source, drain and body terminals of the various MOSFETS discussed with suffixes 1, 2, 3, . . . identifying the respective MOSFET.
Also, for simplicity:
One or more embodiments may rely on the recognition that the threshold voltage VTH of the input transistor can be reduced if a lowest (minimum) input signal level is not sufficient for a particular application.
For instance, in an embodiment as exemplified in
The MOSFET MN3 has its body terminal B3 shorted to its drain terminal D3 and to the body terminal B1 of MN1.
In one or more embodiments, the two MOSFETs MN1 and MN3 may be of the same type so their electrical characteristics are matched, even with different W/L (width/length) sizing applied.
If the input voltage is higher than the threshold voltage VTH of both MOSFETs MN1 and MN3, the body of both these transistors (namely B1 and B3) is tied to GND by MN3.
In the case of MN3, as a result of input voltage VIN dropping near the threshold voltage VTH, the drain current through MN3 will not be sufficient for sinking all the current provided by IBAux and the drain potential of MN3 will start to increase. Because this (drain) node D3 is connected to the bodies (bulks) B1 and B3 of both MOSFETs MN1 and MN3, the potential of these bulk nodes will start to increase.
Due to a resulting body effect the threshold voltage VTH for both the MOSFETs MN1, MN3 will decrease.
As noted, good practice may suggest to size the MOSFETs MN1 and MN3 differently, for instance with the W/L (width/length) ratio of MN1 higher than the W/L ratio for MN3. This will facilitate and early detection of a low input level and application of a body effect as discussed.
The effect of body polarization can be described by the following equation:
Where:
is a constant
The equation reported above proves that applying a positive voltage between the source S and the body B of a MOSFET increases the threshold value VTH, while applying a negative voltage decreases VTH.
One or more embodiments may apply negative polarization (bias) of a source node versus the body. Such a polarization cannot be increased indefinitely insofar as this is limited by the presence of body-source PN junction which becomes forward-polarized when the source terminal is about 0.7V lower than body terminal (at room temperature).
This may put a limit on the amount the body effect can be applied to decrease of VTH.
For instance, in the case of a circuit supplied with VDD=1V and the input voltage VIN swept from 0 to 1V, monitoring the output voltage VOUT in both cases (without body control and with body control) shows the following.
For a standard amplifier without body control (see
If body control is applied (see
It is observed that for high values of VIN (near VDD, for instance, the body voltage or potential Vbody is nearly zero. At input voltage levels around 600 mV the body potential starts to increase and to apply a body effect to the amplifier. At low levels for VIN the body voltage saturates at about 620 mV due to the forward polarization of body-source junction in the MOSFET. In fact, elementary single-MOSFET amplifiers are used in active mode around the voltage VTH. For (much) higher values of VIN, the amplifier output will saturate near zero voltage.
As exemplified in
In that respect, it is again recalled that like elements are indicated with like symbols (for instance G, S, D, B) throughout the figures, thus making it unnecessary to repeat (in respect of
As exemplified in
As exemplified in
As exemplified in
If the IN+ voltage is sufficiently high for normal operation, the bodies MN1, MN2 and MN3 are tied to GND via the current path (drain D3) of MN3 and the circuit operates without body polarization.
If the voltage at IN+ drops near the threshold VTH of MN3, the drain current of MN3 is not able to sink all the IBAux current and the drain potential of MN3 starts to increase. Also, the body potential (Vbody) of all the three MOSFETs MN1, MN2 and MN3 is increased, thus inducing a body effect which reduces the threshold VTH and facilitates normal operation of the amplifier.
Here again, the body effect has a limit in the forward polarization of the body-source PN junctions in the MOSFETs, with the MOSFET MN3 being of the same type as MN1. Again, good practice may suggest to size MN3 differently from MN1, for instance with W/L of MN1 higher than W/L of MN3. The difference in size will result in a certain difference (delta VGS) in the gate-source voltages of the MOSFETs MN1 and MN3, with the voltage VGS of MN1 being lower. Such a delta voltage will occur at the common tail node (sources of MN1 and MN2), facilitating normal current biasing by the tail generator IBTail.
Operation of a circuit as exemplified in
In case the body effect is not applied (see
In case the body effect is relied upon (see
In a circuit as exemplified in
A circuit as exemplified in
Once again, elements like elements already discussed in connection with the previous figures are indicated with like symbols, and a corresponding description will not be repeated here for brevity.
In embodiments as exemplified in
In those circumstances where such a voltage drop at MN1 is found to be insufficient to facilitate correct current mirroring (which, for instance, may be due to VDD being insufficient, that is undesirably low) the possibility again exists of resorting to the body effect in order to increase the body voltage (Vbody) and inducing a reduction in the threshold voltage VTH.
A circuit as exemplified herein may comprise:
In a circuit as exemplified herein (see, for instance,
In a circuit as exemplified herein (see again, for instance,
In a circuit as exemplified herein the at least one body voltage control MOSFET may be of a same type, n-channel or p-channel, of said MOSFET.
A circuit as exemplified herein (see, for instance, the differential arrangement of
wherein:
In a circuit as exemplified herein (see, for instance,
In a circuit as exemplified herein (see again for instance
wherein the first body voltage control MOSFET and the second body voltage control MOSFET have respective first (for instance, B3′) and second (for instance, B3″) body terminals jointly coupled to the body terminal of said MOSFET and to the further body terminal of said further MOSFET (MN2).
In a circuit as exemplified herein (see again, for instance,
In a circuit as exemplified herein the first body voltage control MOSFET and the second body voltage control MOSFET may be of a same type, n-channel or p-channel, of said MOSFET.
A circuit as exemplified herein (see, for instance, the current-mirror arrangement of
wherein:
In a method of operating a MOSFET as exemplified herein, having source and drain terminals with a current conduction path therebetween, a gate terminal configured to receive an input signal to facilitate current conduction in said current conduction path as a result of the gate-to-source voltage reaching a threshold, as well as a body terminal,
the method may comprise:
Without prejudice to the underlying principles, the details and embodiments may vary, even significantly, with respect to what has been described by way of example only, without departing from the extent of protection.
For instance, the exemplary embodiments presented here are not exhaustive. Additional embodiments can be identified by skilled person: just to mention one (non-limiting) case in point, one may consider “complementary” embodiments where n-channel MOSFETs are replaced by p-channel MOSFETs and vice versa, that is, one or more embodiments are applicable to complementary solutions replacing n-channel MOSFETS with p-channel MOSFETs and vice versa.
Also, it will be appreciated that the body effect pursued in the embodiments has been explained in connection with the threshold voltage VTH for simplicity, while the gate-source voltage VGS of the MOSFET, which facilitates conduction of a certain drain current, may be considered.
The extent of protection is determined by the annexed claims.
The claims are an integral part of the technical teaching provided herein in respect of the embodiments.
Number | Date | Country | Kind |
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102019000001941 | Feb 2019 | IT | national |
This application is a continuation of U.S. patent application Ser. No. 16/786,182, filed Feb. 10, 2020, which claims the priority benefit of Italian Application for Patent No. 102019000001941, filed on Feb. 11, 2019, the content of which are hereby incorporated by reference in their entireties to the maximum extent allowable by law.
Number | Date | Country | |
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Parent | 16786182 | Feb 2020 | US |
Child | 17362276 | US |