Bandgap references are electronic circuits that ideally provide a fixed output voltage signal used as a reference to other circuitry, such as analog to digital converters (ADCs), voltage regulators, sensors, and the like. Temperature stability of a bandgap reference is often achieved by combining a circuit signal that is proportional to absolute temperature (PTAT) with a signal that is complementary to absolute temperature (CTAT). Existing designs provide an output voltage of about 1.2-1.3 V based on the nominal theoretical 1.22 eV bandgap of silicon at 0° Kelvin based on a voltage difference between two p-n junctions (e.g., ΔVGS). This limits the minimum operating voltage to about 1.4 V in practice. However, stable reference voltages are needed in low-voltage, low-power circuit applications in which supply voltages of 1.0 V or less are available. Existing low-voltage bandgap reference designs are largely incapable of achieving a precision voltage reference from a supply voltage under 1.0 V over a wide temperature range (e.g., −50° C. to +150° C.), while consuming currents below 1 uA. One approach for a low voltage bandgap reference is to use an internal charge pump circuit to boost a low voltage supply to 1.4 V or higher, but this is noisy, adds cost and requires additional circuit area. Other approaches use MOSFET transistors and fractional bandgap references which can operate at low supply voltage levels using current summing circuits. However, these circuits typically suffer from poor accuracy at low currents, have multiple stable operating points at cold temperatures which limit practical operational temperature ranges, and the circuits use large resistors to generate CTAT currents and are thus not area efficient for ultralow power applications. Reverse bandgap circuits can provide robust accuracy across processes, but these approaches also suffer from multiple operating points and are not area efficient. An area efficient approach uses the threshold voltage difference between two transistors (e.g., ΔVT) to generate a Zero Temperature Coefficient (ZTC) reference signal, but this approach suffers from uncontrolled current levels and the accuracy is not robust across processes.
Described examples provide a bandgap voltage circuit with a first circuit to generate an output voltage as a sum of a first voltage with an amplitude that is proportional to absolute temperature, and a first feedback voltage with an amplitude that is complementary to absolute temperature, a second circuit to generate a voltage having an amplitude that is complementary to absolute temperature, a scaling circuit to generate a second feedback voltage with an amplitude that is a fraction of the voltage of the control terminal, and a regulator circuit to regulate the first feedback voltage according to the second feedback voltage by controlling a first input current of the first circuit and a second input current of the second circuit. Example methods include providing a first current to generate a first feedback voltage across a resistor, providing a second current to generate a CTAT voltage across a transistor, scaling the transistor voltage to generate a second feedback voltage, generating an output voltage as a sum of the first feedback voltage, and a PTAT voltage, and regulating the first feedback voltage according to the second feedback voltage by controlling the amplitudes of the first and second currents. Disclosed examples facilitate robust accuracy across multiple processes for generated CTAT and PTAT voltages over wide temperature ranges, along with controlled circuit current levels to provide improved solutions for low-voltage, low-power applications.
In the drawings, like reference numerals refer to like elements throughout, and the various features are not necessarily drawn to scale. In the following discussion and in the claims, the terms “including”, “includes”, “having”, “has”, “with”, or variants thereof are intended to be inclusive in a manner similar to the term “comprising”, and thus should be interpreted to mean “including, but not limited to . . . ” Also, the terms “coupled”, “couple” or “couples” are intended to include indirect or direct electrical or mechanical connection or combinations thereof. For example, if a first device couples to or is coupled with a second device, that connection may be through a direct electrical connection, or through an indirect electrical connection via one or more intervening devices and/or connections.
The self-cascoded transistor circuit 110 is connected between the first input node 114 and the first feedback node 118. The self-cascoded transistor circuit 110 can be any cascode connected transistors, such as the MOSFET transistors 111 and 112 in the example of
The self-cascoded transistor circuit 110 provides the output voltage VREF as a sum of the first feedback voltage VFB1 and a first voltage, in this case the difference between the gate-source voltages VGS of the transistors 111 and 112 (e.g., VREF=VFB1+ΔVGS, where ΔVGS=VGS2−VGS1, VGS1 is the gate-source voltage of the first NMOS transistor 111, and VGS2 is the gate-source voltage of the second NMOS transistor 112). The first voltage ΔVGS is a PTAT voltage that is proportional to absolute temperature. As used herein, PTAT signals (e.g., PTAT voltage and current signals), are electrical signals that increase with increasing temperature in a generally proportional manner, and PTAT circuits are those that have a positive temperature coefficient (PTC). Also, CTAT signals (e.g., CTAT voltage and current signals), are electrical signals that decrease with increasing temperature in a generally proportional manner, and CTAT circuits are those that have a negative temperature coefficient (NTC). The regulator circuit 120 provides the first input current 121 to the first input terminal 114, and the self-cascoded transistor circuit 110 provides the corresponding current 115 that controls the amplitude of the first feedback voltage VFB1 at the first feedback node 118.
The regulator circuit 120 also provides a second input current 122 to the second circuit 102. The second input current 122 has an amplitude I2. The regulator circuit 120 includes a first regulator transistor 124 connected between the supply node 106 and the first input terminal 114 of the self-cascoded transistor circuit 110. In one example, the first regulator transistor 124 is a p-channel MOSFET (e.g., PMOS) transistor with a source connected to the supply node 106, a gate terminal connected to a control node 126, and a source terminal. Other types and forms of mirror circuit transistors can be used in other implementations. The source terminal of the first regulator transistor 124 is connected to the first input terminal 114 to provide the first input current 121 to the first circuit 101.
The regulator circuit 120 also includes an amplifier 128 with an output connected to the control node 126. The amplifier 128 controls the first amplitude I1 of the first input current 121, and the second amplitude I2 of the second input current 122, according to the difference between the first feedback voltage VFB1 and a second feedback voltage VFB2 from the second circuit 102. The amplifier 128 provides a closed-loop that regulates the first feedback voltage VFB1 according to the second feedback voltage VFB2 by controlling the first input and second input currents 121 and 122 provided to the first and second circuits 101 and 102, respectively. The second circuit 102 includes a second input node 130 that connects a second current regulator transistor 132 with a transistor 134 between the supply node 106 and the reference node 108. The second regulator transistor 132 is a p-channel MOSFET (e.g., PMOS) transistor with a source connected to the supply node 106, a gate terminal connected to the control node 126, and a source terminal that provides the second input current 122 to the second circuit 102. In one example, the second regulator transistor 132 is the same size as that of the first regulator transistor 124. In another example, the second regulator transistor 132 is larger than the first regulator transistor 124, such as twice as large.
In one example, the transistor 134 of the second circuit 102 is an NPN, diode connected bipolar transistor, although other types and forms of transistor can be used in different implementations. In the illustrated example, the collector and base control terminal of the transistor 134 are connected to the second input node 130, and the emitter of the transistor 134 is connected to the reference node 108. The diode-connected NPN bipolar transistor 134 provides the base-emitter voltage VBE to the control terminal at the second input node 130 with an amplitude that is complementary to absolute temperature (CTAT). As used herein, PTAT or “proportional to absolute temperature” or “proportional to temperature” characterizes a device or a circuit that provides or controls a signal, such as a current or voltage, in a manner that increases or decreases generally proportional to an increase or decrease in absolute temperature, respectively. For example, the amplitude of a PTAT voltage signal increases with increasing temperature, and decreases with decreasing temperature. Similarly, a transistor or circuit with a PTAT characteristic generates a signal that increases with increasing temperature, and decreases with decreasing temperature. As used herein, CTAT or “complementary to absolute temperature” or “complementary to temperature” characterizes a device or a circuit that provides or controls a signal, such as a current or voltage, in a manner that increases or decreases inversely with an increase or decrease in absolute temperature, respectively. For example, the amplitude of a CTAT voltage signal decreases with increasing temperature, and increases with decreasing temperature. Similarly, a transistor or circuit with a CTAT characteristic generates a signal that decreases with increasing temperature, and increases with decreasing temperature.
The second circuit 102 further includes a scaling circuit 136 coupled between the transistor 134 and the reference node 108. The scaling circuit 136 includes a second feedback node 138 having the second feedback voltage VFB2. In operation, the scaling circuit 136 scales a base-emitter voltage VBE of the diode-connected transistor 134 to provide the second feedback voltage VFB2 with an amplitude KVBE that is a fraction of the voltage VBE of the control terminal 130 (e.g., VFB2=KVBE). The scaling circuit 136 includes a first divider resistor 140 with a resistance R1 connected between the second input node 130 and the second feedback node 138. The first divider resistor 140 includes a first terminal connected to the second input node 130, and a second terminal connected to the second feedback node 138. The scaling circuit 136 also includes a second divider resistor 142 with a resistance R2 connected between the second feedback node 136 and the reference node 108. The second divider resistor 142 includes a first terminal connected to the second feedback node 138, and a second terminal connected to the reference node 108.
The resistive voltage divider circuit formed by the series connection of the resistors 140 and 142 between the control terminal of the transistor 134 and the reference node 108 scales the base-emitter voltage VBE of the diode-connected transistor 134. The second feedback node 138 that joins the resistors 140 and 142 generates the second feedback voltage VFB2 with the amplitude KVBE. In this example, K is a scaling factor representing the ratio R1/(R1+R2). In one example, the resistor 116 of the first circuit 101 has a resistance R2 equal to the resistance R2 of the second divider resistor 142, although not a strict requirement of all possible implementations. Although the illustrated scaling circuit 136 is a resistive divider, other forms and types of scaling circuits can be used in other implementations that generate the second feedback voltage VFB2 is a fraction of the transistor voltage VBE of the second circuit 102.
The scaling circuit 136 provides the second feedback voltage VFB2 at the second feedback node 138. The second feedback node 138 is connected to an inverting input (−) of the amplifier 128. The non-inverting input (+) is connected to the first feedback node 118 to receive the first feedback voltage VFB1. The amplifier 128 includes an output terminal connected to the gate control terminals of the first and second regulator transistors 124 and 132 at the control node 126. The amplifier 128 provides an output voltage according to the difference between the first and second feedback voltages VFB1 and VFB2. The voltage at the control node 126 controls the first amplitude I1 of the first input current 121, and the second amplitude I2 of the second input current 122.
The regulator circuit 120 provides closed loop control of the first input current 121, which in turn affects the current 117 through the first circuit resistor 116. The negative feedback of the scaled CTAT voltage represented by the second feedback voltage (VFB2=KVBE) regulates the current first feedback voltage VFB1 to be generally equal to the second feedback voltage VFB2. As previously mentioned, the output voltage VREF is generated by the first circuit 101 as the sum of VFB1 and the gate-source voltage VGS of the transistor 112 (e.g., VREF=VFB1+VGS). In this regard, the closed-loop regulation of the first feedback voltage VFB1 to be equal to the second feedback voltage (VFB1=VFB2=KVBE) causes the first feedback voltage at the first feedback voltage node 118 to be a CTAT signal that generally decreases with increasing circuit temperature. At the same time, the gate-source difference voltage ΔVGS of the transistors 111 and 112 is a PTAT signal with an amplitude that varies proportional to absolute temperature (e.g., increases with increasing temperature). Thus, the bandgap voltage circuit 100 provides the output voltage VREF with a generally zero temperature coefficient (ZTC) having a generally temperature independent value. In addition, the scaling of the CTAT feedback through the scaling circuit 136 facilitates low-voltage operation of the circuit 100. In addition, the ZTC characteristic of the output voltage VREF is robust across different processes. In these respects, the bandgap voltage circuit 100 of
The current/voltage (I-V) relationship for the self-cascoded MOSFETs (e.g., the transistors 111 and 112 of the self-cascoded circuit 110 in
In these formulas, Cox is a capacitance of the MOSFET gate oxide, Cd is the MOSFET depletion capacitance, Vgs is the gate-source voltage, Vds is the drain-source voltage, VT is the thermal voltage, and Vth is the threshold voltage, where Vds>4.7 VT ensures <1% loss of accuracy. For the same current (e.g., I1 in
VREF=ΔVGS+kVBE≅=k*VBG. (5)
The self-Cascoded MOSFETs 111 and 112 achieve ΔVGS while generally carrying the same current 121 (e.g., the current 121 and the current 115 are substantially equal, other than leakage currents). Consequently, example implementations do not need current mirrors and any associated errors can be mitigated or avoided. Certain examples can include compensation circuitry 150, such as a current source 152 and a current mirror circuit 156, 158, although not required of all possible implementations. The currents generated in the legs of the second circuit (e.g., the bipolar transistor leg, and the resistive divider leg) are CTAT (e.g., the current 122 is determined according to VBE/(R1+R2), where the voltage VBE has a CTAT characteristic). Accordingly, the current 122 decreases with increasing temperature, and increases with decreasing temperature. As discussed below in connection with
Referring also to
In addition
The bandgap voltage circuit 100 facilitates low-voltage operation by scaling down the CTAT voltage VBE generated by the bipolar transistor 134, and adding the scaled CTAT voltage to the PTAT voltage ΔVGS of the self-cascoded sub-threshold MOSFET transistors 111 and 112 through the closed-loop operation of the regulator circuit 120 using the scaled CTAT voltage KVBE as negative feedback. The example circuit 100 operates over a wide temperature range, unlike the current summing bandgap design or other low voltage CMOS reference designs, while maintaining good accuracy across multiple processes, supply voltages and temperatures (robust with respect to PVT). The disclosed examples 100 provides a bandgap design solution with robustness and accuracy, along with the ability to operate at low supply voltages, while providing circuit area economy without charge pump voltage boosting circuitry or other additional circuits.
The example circuit 100 of
In the example of
In one example, the regulator transistors 132 and 124 are sized with a ratio of 1:2 as shown in
Referring now to
The method 500 of
Referring also to
Referring also to
A curve 912 shows the current 117 (I3) through the resistor 116 of the first circuit 101, which establishes the first feedback voltage VFB1. A curve 914 shows the second compensation current 162 (I4) sinked from the first feedback node 118 by the compensation circuit 150 in the example of
The above examples are merely illustrative of several possible embodiments of various aspects of the present disclosure, wherein equivalent alterations and/or modifications will occur to others skilled in the art upon reading and understanding this specification and the annexed drawings. Modifications are possible in the described embodiments, and other embodiments are possible, within the scope of the claims.
Number | Name | Date | Kind |
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6225796 | Nguyen | May 2001 | B1 |
20070109037 | Lin | May 2007 | A1 |
20090295465 | Tripodi et al. | Dec 2009 | A1 |
20100072972 | Yoshikawa | Mar 2010 | A1 |
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