The present invention relates to a precise voltage/current reference circuit that is insensitive to variations in temperature and power supply voltage. More specifically, the present invention relates to a voltage/current reference circuit using a current-mode technique in CMOS technology.
The voltage across resistor 113, designated as ΔVBE, can therefore be defined as follows.
ΔVBE=VBE1−VBE2 (1)
The current I113 through resistor 113 can then be defined as follows.
I113=ΔVBE/R3 (2)
The voltage drop across resistor 112, (i.e., V112), can therefore be defined as follows.
V112=I113×R2=ΔVBE×R2/R3 (3)
Thus, the reference voltage VREF1 can be defined as follows.
VREF1=VBE1+ΔVBE×R2/R3 (4)
The voltage ΔVBE is proportional to the threshold voltage VT. The voltage VBE1 has a negative temperature coefficient of about −2 mV/° C., whereas VT has a positive temperature coefficient of 0.086 mV/° C. As a result, the temperature variation of VREF1 can be compensated by the ratio of R2/R3.
Because PMOS transistors 201–203 are identical, and R1 is equal to R2, the currents I1, I2 and I3 are equal to one another.
I1=I2=I3 (5)
Because the voltage V+ is equal to the voltage V−, the current through resistor 211 (i.e., I1B) is equal to the current through resistor 212 (i.e., I2B).
I1B=I2B (6)
As a result, the current through bipolar transistor 221 (i.e., I1A) is equal to the current through resistor 213 and bipolar transistor 222 (i.e., I2A)
I1A=I2A (7)
The current I2A through resistor 213 can be defined as follows. This current I2A is proportional to the threshold voltage VT.
I2A=ΔVBE/R3 (8)
The current I2B through resistor 212 can be defined as follows. This current I2B is proportional to VBE1.
I2B=VBE1/R2 (9)
Current I3 can therefore be defined as follows.
I3=I2=I2A+I2B (10)
As a result, the output reference voltage VREF2, which is equal to the current I3×R4, can be defined as follows.
VREF2=R4×(ΔVBE/R3+VBE1/R2) (11)
As described above, the voltage ΔVBE is proportional to the threshold voltage VT, which has a positive temperature coefficient of 0.086 mV/° C., and the voltage VBE1 has a negative temperature coefficient of about −2 mV/° C. Thus, the temperature variation of VREF2 can be compensated by the resistance ratio R2, R3 and R4.
Moreover, as described above, reference circuits 100 and 200 are both voltage references. If a current reference is needed, a voltage-to-current conversion circuit is typically used, wherein the reference voltage is applied to a resistor, thereby creating an associated reference current IREF. However, such a resistor has a positive temperature coefficient. Thus, while the reference voltage may be temperature insensitive, the reference current will vary with variations in temperature, due to the temperature dependence of the resistor. The process variation of the resistor is a major factor that degrades the precision of the current reference.
It would therefore be desirable to have a reference circuit capable of generating both a reference voltage and a reference current that are insensitive to variations in both temperature and power supply voltage. It would further be desirable for this reference circuit to have a single steady-state operating point.
Accordingly, the present invention provides a reference circuit that includes a first bipolar transistor that exhibits a first base-to-emitter voltage VBE1, and a second bipolar transistor that exhibits a second base-to-emitter voltage VBE1, wherein VBE1 is greater than VBE2. The voltage VBE1 is applied a one terminal of a first resistor, and the voltage VBE2 is applied to the other terminal of the first resistor, such that a voltage of VBE1−VBE2 is applied across the first resistor. The first resistor has a resistance R1, such that a first current equal to (VBE1−VBE2)/R1 flows through this first resistor.
A first MOS transistor is configured to supply the first and second currents to the first and second resistors. As a result, the first MOS transistor carries a current equal to the sum of the first and second currents, or (VBE1−VBE2)/R1+VBE1/R2. A second MOS transistor, having a current mirror configuration with respect to the first transistor, directly provides a reference current equal to (VBE1−VBE2)/R1 +VBE1/R2. By properly selecting the ratio of resistances R1 and R2, the reference current can be made insensitive to variations in temperature and power supply voltage.
A third transistor, having a current mirror configuration with respect to the first transistor, provides a current equal to the reference current (i.e., (VBE1−VBE2)/R1 +VBE1/R2) to a third resistor having a resistance R3. This third resistor is connected in series with a third bipolar transistor that exhibits a third base-to-emitter voltage VBE3. As a result, the voltage drop across the third resistor and the third bipolar transistor is equal to VBE3+(R3×(VBE1−VBE2)/R1+R3×VBE1/R2). This voltage drop is used as a reference voltage. By properly selecting the ratio of the resistances R1, R2 and R3, the reference voltage can be made insensitive to variations in temperature and power supply voltage. Moreover, by properly selecting the ratio of the resistances R1, R2 and R3, the voltage and current reference circuit can be controlled to have a single steady-state operating point.
The present invention will be more fully understood in view of the following description and drawings.
Voltage reference circuit 400 includes PMOS transistors 401–404, operational amplifier 405, resistors 411–414 and PNP bipolar transistors 421–423. The dimensions of PMOS transistors 401–404 are the same. The sources of PMOS transistors 401–404 are coupled to the VDD voltage supply terminal. The drains of PMOS transistors 401 and 402 are coupled to the “−” and “+” input terminals of operational amplifier 405. The input voltages to the “−” and “+” input terminals of operational amplifier 405 are labeled as input voltages V− and V+, respectively. The output terminal of operational amplifier 405 is coupled to the gates of PMOS transistors 401–404. The currents through PMOS transistors 401, 402, 403 and 404 are designated as I1, I2, IREF, and IUNIT, respectively. These currents are all equal to one another.
I1=I2=IREF=IUNIT (12)
Resistor 411 and PNP bipolar transistor 421 are coupled in parallel between the drain of PMOS transistor 401 and the VSS (ground) voltage supply terminal. The base of PNP bipolar transistor 421 is also coupled to the VSS voltage supply terminal. The base-to-emitter voltage of bipolar transistor 421 is designated as voltage VBE1. The input voltage V− is therefore equal to VBE1. Operational amplifier 405 forces the input voltages V− and V+ to be equal, such that the input voltage V+ on the drain of PMOS transistor 402 is also equal to VBE1. The currents through PNP bipolar transistor 421 and resistor 411 are designated as current I1A and current I1B, respectively. Note that currents I1, I1A and I1B exhibit the following relationship.
I1=I1A+I1B (13)
Resistor 412 and the series combination of resistor 413 and PNP bipolar transistor 422 are coupled in parallel between the drain of PMOS transistor 402 and the VSS voltage supply terminal. The base of PNP bipolar transistor 422 is also coupled to the VSS voltage supply terminal. The base-to-emitter voltage of bipolar transistor 422 is designated as voltage VBE2. The current through resistor 413 and PNP bipolar transistor 422 is designated as current I2A. The current through resistor 412 is designated as current I2B. Note that currents I2, I2A and I2B exhibit the following relationship.
I2=I2A+I2B (14)
Resistor 413 has a resistance of R, and resistors 411 and 412 each have a resistance of (R×N), where N is an integer.
Resistor 414 and PNP bipolar transistor 423 are coupled in series between the drain of PMOS transistor 403 and the VSS voltage supply terminal. The base of PNP bipolar transistor 423 is also coupled to the VSS voltage supply terminal. The base-to-emitter voltage of bipolar transistor 423 is designated as voltage VBE3. Resistor 414 is a bandgap reference resistor that has a resistance designated RBGR and configured to provide the reference voltage VREF4. The drain of PMOS transistor 403 is connected to resistor 414.
Reference circuit 400 operates as follows. As described above, operational amplifier 405 forces the voltages V+ and V− to be the same (i.e., VBE1). The current I1B through resistor 411 and the current I2B through resistor 412 can therefore be defined as follows.
I1B=I2B=VBE1/(R×N) (15)
Combining Equations (12), (13), (14) and (15) provides the following current relationship.
I1A=I2A (16)
The voltage across resistor 413, designated as ΔVBE, can be defined as follows.
ΔVBE=V+−VBE2=VBE1−VBE2 (17)
The current I2A through resistor 413 can therefore be defined as follows.
I2A=ΔVBE/R (18)
From Equations (14), (15) and (18), the current I2 can be defined as follows.
I2=ΔVBE/R+VBE1/(R×N) (19)
The term ΔVBE has a positive temperature coefficient, the term VBE1 has a negative temperature coefficient and the resistance R has a positive temperature coefficient. As a result, the temperature variation of current I2 can be compensated by the resistor ratio N. The current I2 is mirrored to PMOS transistor 404 as the reference current IUNIT. Thus, PMOS transistor 404 directly provides the desired reference current IUNIT, which is insensitive to variations in temperature. Note that the resistor ratio N is selected to compensate the temperature variation of the current, not the voltage. As a result, the current reference IUNIT can be generated directly.
Circuit 400 also enables a reference voltage VREF4 to be generated. The reference voltage VREF4 can be defined as follows.
VREF4=VBE3+IREF×RBGR (20)
Because the current IREF is equal to the current I2, equation (20) can be rewritten as follows.
Because ΔVBE has a negative temperature coefficient and RBGR has a positive temperature coefficient, the reference voltage VREF4 can be independent of temperature when the resistor ratio N is properly selected. Moreover, the reference voltage VREF4 is determined by the resistance ratio RGBR/R, which is not significantly influenced by the absolute value of the resistances. In the foregoing manner, PNP bipolar transistor 423 and bandgap reference resistor 414 enable the generation of a voltage reference VREF4 that is insensitive to temperature variation.
Because voltage and current reference circuit 500 (
Reference circuit 500 operates in a manner similar to reference circuit 400, with the differences noted below. As described above, operational amplifier 405 forces the voltages V+ and V− to be the same (i.e., VBE1). The current I2B′ through resistor 512 can therefore be defined as follows.
I2B′=2×VBE1/(R×N) (23)
The current I2A through resistor 413 can be defined as follows. (See, Equation (18) above)
I2A=ΔVBE/R (24)
From equations (23) and (24), the current I2′ through PMOS transistor 402 can be defined as follows.
I2′=ΔVBE/R+2×VBE1/(R×N) (25)
The current I2′ is reflected to transistor 404 as the reference current IUNIT′. The term ΔVBE has a positive temperature coefficient, and the term VBE1 has a negative temperature coefficient and the resistance R has a positive temperature coefficient. As a result, the temperature variation of current IUNIT′ can be compensated by the resistor ratio N. Thus, current IUNIT′ is insensitive to variations in temperature. Note that the resistor ratio N is selected to compensate the temperature variation of the current, not the voltage. As a result, the current reference IUNIT′ can be generated directly.
Circuit 500 also enables a reference voltage VREF5 to be generated. The reference voltage VREF5 can be defined as follows.
VREF5=VBE3+IREF′×RBGR (26)
Because the current IREF′ is equal to the current I2′, equation (26) can be rewritten as follows.
VREF5=VBE3+[ΔVBE/R+2×VBE1/(R×N)]×RBGR (27)
VREF5=VBE3+RBGR×ΔVBE/R+2RBGRx×VBE1/(R×N) (28)
Because ΔVBE has a negative temperature coefficient and RBGR has a positive temperature coefficient, the reference voltage VREF5 can be independent of temperature when the resistor ratio N is properly selected. Moreover, the reference voltage VREF5 is determined by the resistance ratio RGBR/R, which is not significantly influenced by the absolute value of the resistances. In the foregoing manner, PNP bipolar transistor 423 and bandgap reference resistor 414 enable the generation of a voltage reference VREF5 that is insensitive to temperature variation.
In the foregoing manner, the reference circuits 400 and 500 provide both current and voltage references. Both are insensitive to the variations of temperature and power supply. The typical variation of such a circuit is less than +/−10%, which is limited by the process variation. This is an improvement over the prior art reference circuits 100 and 200, which exhibit a +/−30% variation in associated reference currents.
Although the invention has been described in connection with several embodiments, it is understood that this invention is not limited to the embodiments disclosed, but is capable of various modifications, which would be apparent to a person skilled in the art. Thus, the invention is limited only by the following claims.
Number | Date | Country | Kind |
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03 1 54092 | Aug 2003 | CN | national |
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Number | Date | Country | |
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20050035814 A1 | Feb 2005 | US |