1. Field of the Invention
This invention relates to semiconductor voltage reference circuits and, more particularly, to bandgap reference circuits.
2. Description of the Related Art
Accurate DC voltage references are ubiquitous building blocks in analog circuit design. Many circuit systems, especially data converters, depend on a stable well-defined voltage reference to achieve performance requirements across variations in process technology, supply voltage, and temperature (PVT) during circuit operation. One such voltage reference is known as a bandgap voltage reference. This class of voltage references typically provides a very stable DC voltage across PVT variation. Temperature-independent behavior of the bandgap output voltage is achieved by appropriately summing two voltage characteristics with temperature coefficients of opposite polarity.
As semiconductor processing technology advances and device geometries continue to get smaller, designing a bandgap reference with very small output voltage variation is increasingly challenging, particularly in deep-submicron CMOS technologies, whether in bulk or silicon-on-insulator (SOI) substrates. The impact of random process variability on circuit behavior is only getting worse as integrated circuit (IC) devices scale to smaller physical dimensions. Moreover, the ability to accurately predict variation in circuit performance using Monte Carlo simulations, for example, is increasingly handicapped by limitations in device variation models and limited characterization of device variation. This may be especially true in cutting-edge products with long design cycles, such as microprocessors, where circuits are designed using extrapolative models to enable time-consuming technology development to take place concurrently. As a result, in many cases, representative variation data is not available during the design process.
Further, conventional complimentary metal oxide semiconductor (CMOS) bandgap reference circuits typically produce a reference voltage of 1.2-1.3V using supply voltages of 1.5V and higher. However, this is unacceptable if the voltage reference needs to be generated using supply voltages near 1.2V or lower. Accordingly, it has become commonplace to build what is referred to as fractional sub-supply bandgap reference circuits. One such conventional sub-supply bandgap reference circuit is shown in
Turning to
From the circuit of
where S=current mirror scaling factor for output current leg
ΔVD=voltage difference between diodes D1 and D2
VD1=voltage across diode D1
η=diode ideality factor, approximately 1
kB=Boltzmann constant=8.617×10−5 eV/K
q=electronic charge=1.602×10−19 Coulomb
N=number of identical parallel D1 diodes to form D2
The near-temperature-independent behavior of the bandgap output voltage is achieved by appropriately choosing a weighted sum of ΔVD (with a voltage characteristic that is proportional to absolute temperature or “PTAT”) and VD1 (with a voltage characteristic that is complementary to absolute temperature or “CTAT”) using a ratio of resistances (R1, R2, and R3) such that the PTAT behavior compensates for the CTAT behavior.
The circuit 100 may work well in some semiconductor technologies, however, when implemented in a deep-submicron CMOS technology, the sub-supply bandgap reference circuit 100 of
More particularly, in semiconductor technologies such as 65 nm SOI CMOS technology and beyond (e.g., 45 nm, 32 nm, etc.), the current mismatch between transistors M1, M2, and M3 (and more specifically between transistors M1 and M2) is of particular concern. Given the significance of diode series resistance, the bias currents through diodes D1 and D2 must be relatively small (e.g., in the range of 1 to 10 μA) to maintain matched η's between the diodes. These small bias currents force the gate overdrive, (i.e., VGS-VT, of transistors M1 and M2) to be relatively small, thereby making the drain currents I1 and I2 of transistors M1 and M2 more susceptible to VT variation. The resulting variation in output reference voltage could be unacceptably high in some systems.
Various embodiments of a pseudo bandgap voltage reference circuit are disclosed. In one embodiment, a reference voltage circuit includes a first transistor and a second transistor, each coupled to a supply voltage node. The circuit also includes an amplifier circuit coupled to a gate terminal of each of the first and the second transistors, a current source coupled to the supply voltage node, and a first diode coupled between the current source and a ground reference node. A first input of the amplifier circuit is coupled to a node between the current source and the first diode. In addition, a first terminal of the first transistor is coupled to a second input of the amplifier circuit in a feedback loop configuration. Also, an output reference voltage is developed at an output node coupled to a second terminal of the second transistor. Further, an output current of the current source is independent of a current flowing through the first terminal of the first transistor.
While the invention is susceptible to various modifications and alternative forms, specific embodiments thereof are shown by way of example in the drawings and will herein be described in detail. It should be understood, however, that the drawings and detailed description thereto are not intended to limit the invention to the particular form disclosed, but on the contrary, the intention is to cover all modifications, equivalents, and alternatives falling within the spirit and scope of the present invention as defined by the appended claims. It is noted that the word “may” is used throughout this application in a permissive sense (i.e., having the potential to, being able to), not a mandatory sense (i.e., must).
Referring to
It is noted that in various embodiments, the current reference IRef may be implemented in a variety of ways. For example, in one embodiment, the current source IRef may be implemented as a simple resistor, while in other embodiments the current source IRef may be implemented as a current mirror. It is further noted that the designations “source” and “drain” of the transistors may be interchanged in some implementations as desired.
In one embodiment, the PBG circuit 200 may overcome a current mismatch between currents I1 and I2 in the sub-supply bandgap reference of
In the implementation of the conventional sub-supply bandgap reference circuit of
VOS=the amplifier's input referred offset voltage
η1 and η2=ideality factors for diodes D1 and D2 respectively
ID1 and ID2=current in diodes D1 and D2 respectively
α=ratio of transistor currents M1 over M2 (due to mismatch it is not 1.0)
λ=ratio of diode currents ID1 over ID2 (due to M1 and M2, and mismatches)
The generated output voltage VRef may be approximated by equation 2
Accordingly, since perfect device matching in the actual implementation of the PBG circuit 200 is also not likely, IREF (which is I1, or ID3) is targeted to be
and if that is achieved, the reference voltage may be shown to be
which is identical to the sub-supply bandgap reference voltage of equation 1. Thus, the nominal reference function provided by the PBG circuit 200 is the substantially the same as a conventional sub-supply bandgap reference circuit 100 of
However due to process and other factors, there may be deviation from the desired values, and the sub-supply deviation from the desired reference current may be denoted as
The deviation in current from ideal in diode D3 will result a deviation in the current in diode D4 from desired as well, and may be denoted as
Then by definition,
The output reference voltage for the PBG circuit 200 may be approximated by
The main difference between equations (2) and (8) is that in equation (2) the α scaling factor is in front, and the factor λ in equation (8) can be significantly larger than that in (2) and still provide smaller deviation in VRef. The following is an exemplary illustration of a result of this difference. In the conventional circuit of
This would yield an output voltage VREF≈600 mV.
Now a 10% device mismatch between transistors M1 and M2 of
As mentioned above, there may also be mismatches in the PBG circuit 200. For example, it is not easy to make the reference current IREF exactly equal to
in the PBG circuit 200. Assume IREF is off by a factor of 2. If δ=−0.5, then σ=−0.216, and λ≈0.64. The output reference voltage is then off from ideal (e.g., IREF=ID4) by 0.5×7.5×25 mV×ln(0.64)≈−41 mV. Thus, even with a very large IREF deviation from an ideal value, the output voltage change in the PBG circuit 200 is smaller than a corresponding voltage change would be in the circuit of
Thus, even with a mismatch in IREF of over 20%, the corresponding reference voltage difference may only be 0.5×7.5×25 mV×ln(0.8)≈−21 mV. This example illustrates that the PBG circuit 200 may provide a superior reference to the conventional sub-supply bandgap reference circuit of
In the PBG circuit 200 of
It is contemplated that in other embodiments, the PBG circuit 200 may have other specific implementations. For example, in one alternative embodiment, for designs that need improved power supply noise rejection, the AC output resistance of M5 can be increased with a cascading or common-gate stage. In another alternative embodiment, to achieve a more constant VREF across PVT variation, the output current can be trimmed by implementing M5 as a number of parallel devices thereby making the current scaling factor S adjustable. The number of parallel devices to activate may be determined for a particular process condition. This is a deterministic form of compensation that can be specified a priori for subsequent circuits after initial silicon characterization, unlike dealing with random device variation which is clearly not deterministic.
Referring to
Although the embodiments above have been described in considerable detail, numerous variations and modifications will become apparent to those skilled in the art once the above disclosure is fully appreciated. It is intended that the following claims be interpreted to embrace all such variations and modifications.