The technical field of the present application relates to bandgap circuits in general, and more particularly, to bandgap compensation circuits.
In analog circuit design, it may be difficult to obtain precise voltages or measurements because analog components have many parameters that vary with process, temperature, and/or or power supplied. Therefore, one or more reference voltages for an integrated circuit may be generated from a bandgap reference voltage circuit. If, however, the bandgap reference voltage is not accurate due to variations in particular of the temperature, then all reference voltages derived from the bandgap reference voltage will also be inaccurate. This could induce substantial errors in the operation of the integrated circuit.
The second order bow of a standard bandgap voltage reference significantly reduces the accuracy of the bandgap voltage over an extended temperature operating range. The second order bow also may add noise on the reference voltage when the bandgap cell is operating at low or high temperatures.
There exists a need for a less temperature dependent bandgap.
According to an embodiment, a bandgap circuit may comprise a first order compensated bandgap unit generating a first output voltage, and a second order compensation circuit adding a second output voltage to the first output voltage and comprising a first metal oxide semiconductor (MOS) transistor coupled in parallel with a first resistor, wherein the first MOS transistor is biased with an inverse proportional to absolute temperature (PTAT) voltage.
According to a further embodiment, the first order compensated bandgap unit may comprise first and second bipolar transistors. According to a further embodiment, the second order compensation circuit may comprise a first controllable current source whose output is coupled with a reference potential via a diode connected third bipolar transistor connected in series with a diode connected second MOS transistor, wherein the output of the first current source controls said first MOS transistor. According to a further embodiment, a second order compensation voltage may be added by coupling the second order compensation circuit in series with the first order compensated bandgap unit.
According to a first type of embodiments, the first order compensated bandgap unit may comprise a current mirror being coupled with the first and second bipolar transistors, second and third resistors coupled in series between the first bipolar transistor and a reference potential, wherein the second bipolar transistor is connected with a node between the second and third resistor, and an operational amplifier whose inputs are connected with nodes between the current mirror and the first and second bipolar transistors, respectively and whose output controls the first and second bipolar transistors. According to a further embodiment, the current mirror can be formed by MOS transistors. According to a further embodiment, the controllable current source can be formed by a MOS transistor and coupled with the current mirror.
According to another type of embodiments of the bandgap circuit, the first order compensated bandgap unit may comprise a second controllable current source being coupled with the first bipolar transistor via series connected second and third resistors and being coupled with the second bipolar transistor via a fourth resistor, and comprises an operational amplifier having a first input coupled with a node between the second and third resistors and a second input coupled with a node between the fourth resistor and the second bipolar transistor and an output which controls the first and second controllable current sources.
According to yet another type of embodiments of the bandgap circuit, the second order compensation circuit may comprise first and second controllable current sources and a diode connected second MOS transistor connected in series with a diode connected first bipolar transistor between said first controllable current source and a reference potential, wherein the node between the first controllable current source and the MOS transistor controls said first MOS transistor and wherein the second controllable current source is coupled with the parallel coupled first MOS transistor and first resistor. According to a further embodiment, a second order compensation voltage can be added by controlling said bipolar transistors of said first order compensated bandgap unit with the second order compensation voltage. According to a further embodiment, the first order compensated bandgap unit may comprise a third controllable current source coupled with ground through a first branch comprising a series connection of second and third resistors and the first bipolar transistor and through a second branch comprising a series connection of a fourth resistor and the second bipolar transistor, a operational amplifier whose input is coupled with a node between the second and third resistor and a node between the fourth resistor and the second bipolar transistor, wherein an output of the operational amplifier controls said first, second and third current source. According to a further embodiment, the first, second and third controllable current sources can be formed by MOS transistors.
According to another embodiment, a method for generating a reference voltage, may comprise the steps of generating a first order compensated bandgap voltage, and generating a second order compensation voltage using a first metal oxide semiconductor (MOS) transistor coupled in parallel with a first resistor, wherein the first MOS transistor is biased with an inverse proportional to absolute temperature (PTAT) voltage; and adding the second order compensation voltage to the first order compensated bandgap voltage.
According to a further embodiment of the method, the MOS transistor may be operated in the triode region. According to a further embodiment of the method, the second order compensation voltage can be generated by controlling the first MOS transistor with a control signal generated by a controllable current feeding a diode connected third bipolar transistor connected in series with a diode connected second MOS transistor. According to a further embodiment of the method, the second order compensation voltage can be generated by feeding a first current to the parallel coupled first MOS transistor and first resistor and controlling the first MOS transistor by a signal generated by a second current feeding a diode connected second MOS transistor connected in series with a diode connected first bipolar transistor.
According to yet another embodiment, a bandgap circuit may comprise a first order compensated bandgap unit comprising first and second bipolar transistors generating a first output voltage, and a second order compensation circuit adding a second output voltage to the first output voltage and comprising a first metal oxide semiconductor (MOS) transistor coupled in parallel with a first resistor, wherein the first MOS transistor is biased with an inverse proportional to absolute temperature (PTAT) voltage, wherein the second order compensation circuit comprises a controllable current source and a diode connected third bipolar transistor connected in series with a diode connected second MOS transistor between the controllable current source and a reference potential, wherein a voltage created by means of the controllable current source controls the first MOS transistor.
According to a further embodiment of the bandgap circuit, a second order compensation voltage can be added by coupling the second order compensation circuit in series with the first order compensated bandgap unit. According to a further embodiment of the bandgap circuit, the first order compensated bandgap unit may comprise a current mirror being coupled with the first and second bipolar transistors, second and third resistors coupled in series between the first bipolar transistor and a reference potential, wherein the second bipolar transistor is connected with a node between the second and third resistor, and an operational amplifier whose inputs are connected with nodes between the current mirror and the first and second bipolar transistors, respectively and whose output controls the first and second bipolar transistors. According to a further embodiment of the bandgap circuit, the first order compensated bandgap unit may comprise a third controllable current source coupled with ground through a first branch comprising a series connection of second and third resistors and the first bipolar transistor and through a second branch comprising a series connection of a fourth resistor and the second bipolar transistor, a operational amplifier whose input is coupled with a node between the second and third resistor and a node between the fourth resistor and the second bipolar transistor, wherein an output of the operational amplifier controls the first, second and third current source. According to a further embodiment of the bandgap circuit, a second order compensation voltage can be added by controlling the bipolar transistors of the first order compensated bandgap unit with the second order compensation voltage.
A more complete understanding of the present embodiments and advantages thereof may be acquired by referring to the following description taken in conjunction with the accompanying drawings, in which like reference numbers indicate like features, and wherein:
a and b shows further embodiments of a bandgap circuit;
a and b show conventional bandgap circuits; and
Preferred embodiments and their advantages are best understood by reference to
a illustrates a conventional bandgap generation circuit. Two current sources are formed by current mirror consisting of MOSFET transistors 105 and 115. The first branch of this current mirror includes a first bipolar transistor 140, that has a size of A (A>1), which has its emitter node 142 coupled to ground via two in series connected resistors 145 and 150, its base connected to the output voltage node 125 and its collector connected to a current mirror input node 107. The second branch includes a second bipolar transistor 135, that has a size of 1, which has its emitter node 147 coupled to ground through resistor 150. Thus the emitter of transistor 135 is connected to the mid point 147 between resistors 145 and 150. An operational amplifier is connected to the collectors of the first and second bipolar transistor 140, 135 wherein its output is coupled with the base of both bipolar transistors 135, 140 and with an output terminal 125 carrying the reference output voltage.
The PTAT current generator comprises MOS current mirror 105 and 115, the two bipolar 135 and 140, the resistor 145 and amplifier 130. It can be shown that the 1st order estimate of current flowing in each branch of the current mirror is equal to
T*ln(A)*Ut/R145,
where T is the absolute temperature in Kelvin, ln(A) is the natural logarithm of A, Ut the thermodynamic voltage is equal to 86 μV, and R145 is the value of resistor 145. Since ln(A)*Ut/R145 is a circuit constant that depends on A and R145, the current flowing in each branch of the current mirror is proportional to the absolute temperature.
It can be noted that there is a junction voltage, the base emitter junction between the output node 125 and mid resistor point node 147. Thus, the voltage difference between the output node 125 and node 147 decreases by 2 mV/K.
The PTAT voltage is achieved forcing the sum of the two PTAT currents into the resistor 150. The voltage across resistor 150 becomes 2*T*86 μV*ln(A)*(R150/R145) where R150 is the value of resistor 150. Therefore when the (R150/R145) resistor ratio is set to 1 mV/(86 μV*ln(A)), the 2 mV/K PTAT voltage is achieved on node 147.
The voltage on the output node 125 is the sum of bipolar 135 base emitter junction voltage (that decreases by 2 mV/K) with the voltage on node 147. Thus it becomes independent of the temperature when the (R150/R145) resistor ratio is set to 1 mV/(86 μV*ln(A)).
In practice both the PTAT current and junction voltage have higher order components that induce the well known bell characteristic of standard bandgap cell. These higher order components induce a few mV variation of the bandgap voltage across the standard −50° C. to 150° C. operating range of the bandgap cell. This isn't an issue for many applications. However when high accuracy is required the bell amplitude needs being minimized. Cancelling the 2nd order component (that dominates in higher order components) already dramatically improves the bandgap voltage accuracy over temperature.
The conventional way for cancelling the 2nd order component of the bandgap voltage is using a material that has a positive temperature coefficient for R150. Unfortunately it's almost impossible having a material that gives the correct positive temperature coefficient for R150. Usually the available material has a too high positive temperature coefficient. Thus the R150 is realized by a series combination of two different materials resistors R150a and R150b in order to achieve the correct value for the residual temperature coefficient as shown in
The aforementioned problems are solved, and other and further benefits achieved by compensating the typical bow of a bandgap circuit by generating a compensation voltage that has a low first order component with respect to the 2nd order component. According to the teachings of this disclosure, a simple and universal solution to bandgap bow may be applied to most types of bandgap circuit architectures, and may be applied to existing bandgap cells with only minor modifications thereto by adding a small amplitude (10-20 mV maximum) concave voltage to the initial bandgap voltage for compensating its second order convex behavior.
According to various embodiments, this can be achieved by using a MOS device operated in the triode region. A MOS device used in the triode region has its gate voltage biased by an inverse PTAT voltage. Thus its “on” resistance dramatically increases with the temperature. This emulates a very high positive temperature coefficient for the “on” resistor. Biasing the resistor with a PTAT current generates a voltage that has a prominent 2nd order component.
As mentioned above, such a concave (2nd order) voltage can be achieved, for example, through a metal oxide semiconductor (MOS) transistor used as variable resistance versus temperature. The gate voltage of the MOS transistor device is biased via an inverse Proportional To Absolute Temperature (PTAT) voltage, thereby inducing a concave behavior of the “on resistance” with the temperature which mostly comprises a second order components. This concave behavior induces a concave voltage drop on the “on resistance” that dramatically reduces the initial second order convex behavior of the bandgap cell. In practice the induced concave voltage has too much gain at high temperature. This is why it is used in parallel with a standard resistance that clamps the gain at high temperatures.
a shows another standard bandgap cell with the added compensation circuit as introduced in
Usually the there is no access to the collector of vertical PNP devices 255 and 260 since the substrate is their collector. This is why the compensation voltage needs being applied through their base terminal. But the base current of vertical PNP transistor 255 and 260 is usually very small compared to their emitter current. Moreover, the base current has a strong temperature dependency (usually it decreases with the temperature) and has dispersion over process. This renders the compensation inefficient without an external bias current. This is why the extra bias source 210 is required with such devices.
However, when floating bipolar (or diode) devices are available, the compensation circuit can be connected as shown in
The gate voltage of MOSFET transistor 160 in
While embodiments of this disclosure have been depicted, described, and are defined by reference to example embodiments of the disclosure, such references do not imply a limitation on the disclosure, and no such limitation is to be inferred. The subject matter disclosed is capable of considerable modification, alteration, and equivalents in form and function, as will occur to those ordinarily skilled in the pertinent art and having the benefit of this disclosure.
This application claims the benefit of U.S. Provisional Application No. 61/245,908 filed on Sep. 25, 2009, entitled “SIMPLE UNIVERSAL SECOND-ORDER TEMPERATURE COMPENSATION TECHNIQUE FOR BANDGAP CELLS”, which is incorporated herein in its entirety.
Number | Name | Date | Kind |
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5291122 | Audy | Mar 1994 | A |
6407622 | Opris | Jun 2002 | B1 |
7602236 | Jo | Oct 2009 | B2 |
7612606 | Marinca | Nov 2009 | B2 |
Number | Date | Country | |
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20110074495 A1 | Mar 2011 | US |
Number | Date | Country | |
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61245908 | Sep 2009 | US |