CMOS compatible band gap reference

Information

  • Patent Grant
  • 6657480
  • Patent Number
    6,657,480
  • Date Filed
    Friday, July 20, 2001
    23 years ago
  • Date Issued
    Tuesday, December 2, 2003
    20 years ago
  • Inventors
  • Original Assignees
  • Examiners
    • Callahan; Timothy P.
    • Englund; Terry L.
    Agents
    • Townsend and Townsend and Crew LLP
    • Cahill; Steven J.
Abstract
A CMOS low noise band gap reference circuit outputs a substantially constant reference voltage VREF. The band gap reference circuit has an amplifier that includes a differential pair of bipolar junction transistors and a feedback circuit that adjusts its current to compensate for variations in the bias current through the circuit. The band gap reference circuit provides an output reference voltage VREF that is substantially constant over a range of temperature and a range of supply voltage.
Description




BACKGROUND OF THE INVENTION




The present invention relates to band gap reference circuits, and more particularly, to band gap reference circuits that maintain a constant output voltage over a range of temperature and bias current.




A band gap reference circuit provides a constant output reference voltage V


REF


. Problems may arise if the output reference voltage V


REF


varies even by a small amount such as a few hundred millivolts over a range of temperature or bias current. Therefore, it is desirable to provide a band gap reference circuit that provides an output reference voltage V


REF


that is substantially constant over a range of temperature and bias current.




Previously known standard CMOS band gap reference circuits typically include an amplifier that comprises a differential pair of p-channel MOS transistors. V


REF


is determined by the voltage at the gate of one of the p-channel MOS transistors. Excess charge carriers can become trapped in the silicon to silicon dioxide (SiO


2


) interface in MOS transistors. The excess charge may cause variations in the threshold voltages of the MOS transistors in the differential pair of the amplifier. For example, the threshold voltages of the two MOS transistors in the differential pair may differ by more than 5 mV. This difference introduces an offset voltage into the amplifier which appears at V


REF


of the band gap reference circuit. The offset voltage can prevent the band gap reference circuit from being adjusted with trimming resistors so that V


REF


remains constant with temperature changes.




In addition, the charge trapped in the silicon/SiO


2


interface of the differential pair MOS transistors in the band gap reference amplifier can vary over time causing V


REF


to change over time even at a constant temperature. These variations in V


REF


cause undesirable 1/f output noise. Also, the p-channel MOS transistors in the differential pair may introduce thermal noise at V


REF


due to the nature of MOS transistors, which is also undesirable.




A further disadvantage of previously known standard CMOS band gap reference circuits is that they are sensitive to relatively small changes in the supply voltage V


CC


. Small changes in V


CC


cause variations in the bias current through the band gap reference circuit, which can cause undesirable changes in V


REF


.




It would therefore be desirable to provide a less noisy band gap reference circuit in CMOS technology that provides a substantially constant output reference voltage V


REF


over a range of supply voltage and a range of temperature.




BRIEF SUMMARY OF THE INVENTION




The present invention provides CMOS low noise band gap reference circuits that output a substantially constant reference voltage V


REF


. Band gap reference circuits of the present invention have an amplifier that includes a differential pair of bipolar junction transistors. Each of the bipolar junction transistors are coupled to a first or a second plurality of bipolar junction transistors or a first and second plurality of diodes. The first and second plurality of transistors or diodes are coupled to a plurality of resistors. When the temperature of the circuit varies over a range, the change in the voltage drop across the resistors compensates for the change in the voltage drop across the transistors or the diodes so that V


REF


remains substantially constant.




A feedback circuit is coupled to the amplifier. The feedback circuit adjusts its current to compensate for variations in the supply current so that the V


REF


remains substantially constant. The band gap reference circuits of the present invention provide a output reference voltage V


REF


that is substantially constant with variations over a range of temperature and supply voltage. Band gap reference circuits of the present invention may be fabricated using standard CMOS process techniques.











BRIEF DESCRIPTION OF THE DRAWINGS




FIG.


1


. is a schematic of an embodiment of a band gap reference circuit of the present invention;





FIGS. 2A-2B

illustrate top down and cross sectional layout views, respectively, of a CMOS compatible lateral PNP bipolar junction transistor in accordance with the principles of the present invention;





FIG. 2C

illustrates a schematic of the lateral PNP BJT of

FIGS. 2A-2B

;





FIGS. 3A-3B

illustrate top down and cross sectional layout views, respectively, of a CMOS compatible vertical PNP bipolar junction transistor in accordance with the principles of the present invention;





FIG. 3C

illustrates a schematic of the vertical PNP bipolar junction transistor of

FIGS. 3A-3B

; and





FIG. 4

is a schematic of another embodiment of a band gap reference circuit of the present invention.











DETAILED DESCRIPTION OF THE INVENTION




Band gap reference circuit


10


shown in

FIG. 1

is an embodiment of the present invention. Reference circuit


10


receives supply voltage V


CC


from an external voltage source. Bias current source


11


, which has a finite impedance, provides a reference current source that outputs a current equal to 15I to reference circuit


10


. For example, 15I may represent 150 μA at 25° C. Bias current source


11


is proportional to absolute temperature. Therefore, changes in the temperature of circuit


10


or changes in V


CC


cause the current through current source


11


to vary.




The current through bias current source


11


is divided through p-channel MOS transistors M


1


-M


8


and M


11


according to the predetermined proportions which are determined by the relative channel width-to-length (W/L) ratios of MOSFET transistors M


1


-M


8


and M


11


. For example, the W/L ratio of transistors M


1


:M


2


:M


3


:M


4


:M


5


:M


6


:M


7


:M


8


may be 4:1:1:1:1:1:1:1 which provides a current ratio of 4I:I:I:I:I:I:I:I as shown in FIG.


1


. MOS transistor M


11


has a W/L that is eight times the W/L of MOS transistors M


9


and M


10


. Other suitable transistor ratios may be used, if desired, according to the principles of the present invention. In a further embodiment of the present invention, MOSFET transistors M


1


-M


8


may be replaced with PNP bipolar junction transistors that are sized to provide the desired bias current ratio in circuit


10


.




Band gap reference circuit


10


includes PNP bipolar junction transistors (BJTs) Q


1


and Q


2


, which from a differential pair for an amplifier. When the voltages at the bases of Q


1


and Q


2


are equal, a current equal to one half of current I (I′/2) flows through both Q


1


and Q


2


, and n-channel MOS transistors M


9


and M


10


, which form a current mirror.




Circuit


10


also includes PNP BJTs Q


4


-Q


9


. The base of transistor Q


2


is coupled to the output reference voltage Vref, which is determined by the equation (1).








V




REF




=V




R2




+V




BE-Q9




+V




BE-Q7




+V




BE-Q5


  (1)






V


R2


is the voltage drop across R


2


, V


BE-Q9


equals the base-emitter voltage drop across Q


9


, V


BE-Q7


equals the base-emitter voltage drop across Q


7


, and V


BE-Q5


equals the base-emitter voltage drop across Q


5


. The voltage at the base of transistor Q


1


is determined by equation (2).








V




Q1




=V




R1




+V




R2




+V




BE-Q8




+V




BE-Q6




+V




BE-Q4


  (2)






V


Q1


is the base voltage of transistor Q


1


, V


R1


is the voltage drop across resistor R


1


, V


BE-Q8


equals the base-emitter voltage drop across Q


8


, V


BE-Q6


equals the base-emitter voltage drop across Q


6


, and V


BE-Q4


equals the base-emitter voltage drop across Q


4


.




BJTs Q


1


-Q


9


may be CMOS compatible lateral PNP bipolar junction transistors.

FIGS. 2A-2B

illustrate top down and cross sectional views of an embodiment of a CMOS compatible lateral PNP bipolar junction transistor that may be used to form BJTs Q


1


-Q


9


.

FIG. 2C

illustrates a schematic of a lateral PNP BJT. The lateral PNP BJT shown in

FIGS. 2A-2B

includes a P+ emitter diffusion region, an N-well base region, and a P+ lateral collector diffusion region. The lateral PNP BJT of

FIGS. 2A-2B

can be made using standard CMOS process techniques that are used to form a p-channel MOSFET transistor. No new layers or process steps are required. The gate terminal in

FIGS. 2A-2B

is biased so that the parallel PMOS device is kept off. The vertical collector terminal is not used. Lateral PNP BJTs have a relatively high base-to-collector current gain β (e.g., 100).




In a further embodiment, BJTs Q


4


-Q


9


may be compatible vertical PNP bipolar junction transistors.

FIGS. 3A-3B

illustrate top down and cross sectional views of an embodiment of a CMOS compatible vertical PNP bipolar junction transistor that may be used to form BJTs Q


4


-Q


9


.

FIG. 3C

illustrates a schematic of a vertical PNP BJT. The PNP transistor in

FIGS. 3A-3B

includes an emitter P+diffusion region, an N-well base region, and a P+ collector region coupled to the P-substrate. Thus, the collector of the vertical PNP BJT is coupled to the P-substrate. Transistors Q


4


-Q


9


can be vertical PNP BJTS, because their collectors are coupled directly to ground. Transistors Q


1


-Q


3


cannot be vertical PNP BJTS, because their collectors are not coupled directly to ground. The vertical PNP BJT of

FIGS. 2A-2B

can be made using standard CMOS process techniques that are used to form a p-channel MOSFET transistor. Vertical PNP BJTs have a relatively high base-to-collector current gain β (e.g., 500).




BJTs Q


4


, Q


6


, and Q


8


have base-emitter junction areas that are 8 times the base emitter junction areas of BJTs Q


5


, Q


7


, and Q


9


. Therefore, base-emitter voltage V


BE


of each of transistors Q


4


, Q


6


, and Q


8


are 26 mV·ln(8)=54 mV greater than the base-emitter voltages V


BE


of each of transistors Q


5


, Q


7


, and Q


9


. The total voltage drop of V


BE-Q8


+V


BE-Q6


+V


BE-Q4


is 162 mV greater than the total voltage of V


BE-Q9


+V


BE-Q7


+V


BE-Q5


. Therefore, the resistance of resistor R


1


should be selected so that the voltage drop across R


1


equals 162 mV so that the voltage at the base of Q


1


equals the voltage at the base of Q


2


. For example, the voltage drop across R


1


is 162 mV when R


1


is 4.05 kΩ and the current of through R


1


is 40 μA. When the voltages at the bases of Q


1


and Q


2


are equal, circuit


10


is in an equilibrium state and outputs a constant output voltage V


REF


.




When the temperature of circuit


10


increases, the base-emitter junction voltage drops across the bipolar junction transistors Q


5


, Q


7


, and Q


9


decreases, and the voltage drop across resistors R


1


and R


2


increases. When the temperature of circuit


10


decreases, the voltage drop across base-emitter junctions of BJTs Q


5


, Q


7


, and Q


9


increases, and the voltage drop across R


1


and R


2


decreases. If a temperature change in circuit


10


causes a voltage change in V


REF


away from a desired value (e.g., 3.6 volts), a trimming resistor can be added in series or in parallel with resistor R


2


to bring V


REF


back up to the desired value. The trimming resistor can be coupled to R


2


using fusible links that are isolated with respect to ground to reduce parasitic capacitance.




Once circuit


10


has been adjusted to reach a balance point (so that V


REF


is at the desired value), then temperature changes over a range (e.g., −40° C.−125° C.) in circuit


10


do not cause voltage changes in V


REF


. At the balance point of circuit


10


, a change in the voltage drop across the base-emitter junctions of BJTs Q


5


, Q


7


, and Q


9


is offset by a change in the voltage drop across resistor R


1


when the temperature of circuit


10


changes such that the voltage of V


REF


remains substantially constant (e.g., within a few millivolts). Therefore, trimming resistance may be added to circuit


10


to achieve a zero temperature coefficient. If desired, resistor R


1


can be selected at a single temperature to achieve the balance point at which V


REF


remains constant despite changes in temperature. Highly accurate measurements of resistances may be needed to achieve this result in one step.




The base-emitter threshold voltages of BJTs Q


1


and Q


2


are the substantially the same, and therefore a low offset voltage is introduced into V


REF


. Variations in the base-emitter threshold voltages of BJTs are on the order of 100-1000 times less than variations in the threshold voltages of MOS transistors. Circuit


10


uses triple emitter followers Q


4


/Q


6


/Q


8


and Q


5


/Q


7


/Q


9


that provide a three times increase in the delta V


BE


(e.g., 3·54 mV) which reduces the effect of the small input offset voltages and noise voltages that are introduced by Q


1


and Q


2


into V


REF


.




Thus, triple emitter followers Q


4


/Q


6


/Q


8


and Q


5


/Q


7


/Q


9


as shown in

FIG. 1

is preferred. However, in a further embodiment, a first double emitter follower is coupled to the base of Q


1


(e.g., by eliminating transistors Q


4


and M


2


in circuit


10


), and a second double emitter follower is coupled to the base of Q


2


(e.g., by eliminating transistors Q


5


and M


8


). Also, in another embodiment, only a single BJT is coupled between the base of Q


1


and R


1


, and a single BJT is coupled between the base of Q


2


and R


2


(e.g., by eliminating transistors Q


4


, Q


5


, Q


6


, Q


7


, M


2


, M


3


, M


7


and M


8


in circuit


10


).




BJTs Q


1


and Q


2


emit low thermal noise, and therefore, circuit


10


exhibits noise performance levels comparable with bipolar band-gap reference circuits. In addition, BJTs Q


1


and Q


2


do not contain the trapped charge that often exists in prior art MOS differential pairs. Therefore, V


REF


in circuit


10


is stable with time and past use history, and does not contain long term drift components that cause the noise problems associated with variations in trapped charge over time that are caused by MOS differential pairs.




In prior art band gap reference circuits that used an amplifier with a p-channel MOS differential pair, an offset voltage may be included in the value of V


REF


due to variations in the threshold voltages of the differential pair MOS transistors. V


REF


in these circuits is determined by the base-emitter voltage drop across a BJT and the voltage drop across a resistor. When the temperature of the prior art band reference circuit changes, the voltage of V


REF


changes from a desired value due to changes in the voltage drops across the resistor and the BJT. The prior art circuits do not reach a balance point when trimming resistors are added to bring V


REF


back up to the desired value, because the offset voltage introduced by differential pair MOS transistors is included in V


REF


.




V


REF


in the prior art reference circuit cannot remain substantially constant with changing temperature, because it does not reach a point at which the decrease in the voltage drop across the BJT cancels out the increase in voltage drop across the resistor when V


REF


is set at the desired value. The offset in V


REF


introduced by the differential pair MOS transistors may cause a designer to add trimming resistance that cause V


REF


to reach the desired value, but that is to much or too little trimming resistance to reach the balance point at which the effect of temperature changes are canceled out and no longer effect V


REF


.




Circuit


10


of the present invention is also substantially resistant to small first order variations in supply voltage V


CC


. When V


CC


increases, the current output of bias current source


11


increases. A small increase in the current through resistors R


1


and R


2


causes an increase in voltages at the bases of Q


1


and Q


2


. However, the voltage at the base of Q


1


increases more than Q


2


, because the increase in the voltage drop at the base of Q


4


is greater than the voltage drop at the base of Q


5


. Therefore, the current through Q


1


decreases below the current through Q


2


, causing both the gate voltage of M


11


and the current through M


11


to increase. Diode coupled BJT Q


3


is coupled to transistor Ml


11


. The channel width-to-length (W/L) ratio of transistors M


9


and M


10


are designed to be equal. By scaling W/L of M


11


to be eight times the W/L of M


9


or M


10


, VDS of M


10


substantially matches VDS Of M


9


, so that the collector current of Q


3


is approximately eight times larger than the collector current of Q


2


or Q


1


, minimizing any imbalance of Q


1


and Q


2


in the feedback loop.




The current through M


11


is several times the magnitude of the current through M


10


and M


9


. The current through M


11


increases as much as the current through current source


11


increases. Therefore, all of the excess current through current source


11


flows through M


11


, and the current through transistors M


1


-M


8


and resistors R


1


and R


2


remains substantially constant.




In a further embodiment of the present invention, the ratio of the current through transistor M


11


with respect to the current through transistors M


9


/M


10


may be selected to be any suitable value. For example, MOS transistor M


11


may have a W/L that is 20 times the W/L of MOS transistors M


9


and M


10


. In this embodiment, the current through M


11


is 20 times the current through M


9


and M


10


.




When V


CC


decreases, the current output of bias current source


11


decreases. The current through M


11


decreases by the same amount that the current through current source


11


decreases. Substantially all of the current drop through current source


11


is subtracted from the current through M


11


, and the current through transistors M


1


-M


8


and resistors R


1


and R


2


again remain substantially constant. Therefore, transistor M


11


is a feedback circuit that regulates its current so that the current through R


1


/R


2


and Q


4


-Q


9


are substantially constant. This is advantageous, because the feedback circuit causes the voltage drop across resistors R


1


and R


2


to remain substantially constant (e.g., 162 mV), the base voltages of Q


1


and Q


2


to remain substantially equal to each other, and the output voltage V


REF


to remain substantially constant despite small, first order changes in the current through current source


11


. Thus, circuit


10


is desensitized from first order variations in V


CC


.




With respect to base currents of Q


4


and Q


5


, the base current of Q


4


tends to cancel some but not all of the base current of Q


5


. Therefore, the base current of Q


5


does introduce an error term into the circuit


10


with respect to reaching the balance point at which a zero temperature coefficient is achieved. However, the error term introduced by the base current of Q


5


is relatively small and does effect the zero temperature coefficient much. To further ensure that the error term introduced by the base of Q


5


is small, the impedances of R


1


and R


2


should be low relative to the base current of Q


5


, as is the case in the embodiment of FIG.


1


. Also, Q


5


can be a vertical PNP BJT, which has a relatively high base-to-collector current gain (β), which further reduces the error term introduced by the base current of Q


5


.




Parasitic capacitance in the feedback loop of circuit


10


provide sufficient compensation for the loop such that additional frequency compensation need not be added. However, an additional capacitor may be from the base of Q


2


to ground to provide additional noise rejection in V


REF


.




Band gap reference circuit


40


shown in

FIG. 4

is a further embodiment of the present invention. Circuit


40


includes p-channel MOSFETs M


4


-M


6


, n-channel MOSFETs M


9


-M


11


, resistors R


1


and R


2


, current source


11


, and PNP BJTs Q


1


and Q


2


, as with the embodiment of FIG.


1


. Circuit


40


also includes diodes


41


-


46


in place of BJTs Q


4


-Q


9


. Current source


11


outputs a current equal to 7I. Current source


11


provides a current I to each of MOSFETs M


4


-M


6


. A current substantially equal to I flows through diodes


41


-


43


and resistors R


1


and R


2


. A current substantially equal to I also flows through diodes


44


-


46


and resistor R


2


. A total current of


2


I flows through R


2


.




In circuit


40


, diodes


41


-


43


have P-N junction areas that are eight times the P-N junction areas of diodes


44


-


46


. Also, Q


1


has a base-emitter junction area that is eight times the base emitter junction area of Q


2


. Therefore, R


1


should be selected to have a voltage drop of 54 mV·4=216 mV to compensate for the fact that the voltage drop across Q


1


and diodes


41


-


43


is 216 mV greater than the voltage drop across Q


2


and diodes


44


-


46


.




A current of


4


I flows through transistor M


11


. Transistor M


11


has a W/L ratio that is eight times the W/L ratio of each of transistors M


9


and M


10


. The feedback circuit comprising M


11


and Q


3


ensure that a current equal to I/2 flows through each of transistors M


9


and M


10


.




The resistance at R


2


may be selected to achieve a desired value at V


REF


. R


2


may be trimmed to achieve a zero temperature coefficient at which point output signal V


REF


remains constant over a range of temperature as discussed above with respect to FIG.


1


.




In a further embodiment of the present invention, diodes


43


and


46


in circuit


40


may be eliminated, so that the base of Q


1


is coupled directly to diode


42


and the base of Q


2


is coupled directly to diode


45


. In another further embodiment of the present invention, diodes


42


-


43


and diodes


45


-


46


may be eliminated, so that the base of Q


1


is coupled directly to diode


41


, and the base of Q


2


is coupled directly to the diode


44


. In still a further embodiment of the present invention, transistor Q


4


in circuit


10


may be replaced with diode


41


, eliminating transistor M


1


, and transistor Q


5


in circuit


10


may be replaced with diode


44


.




In still a further embodiment of the present invention, PNP BJTs Q


1


-Q


2


and BJTs Q


4


-Q


9


may be replaced with NPN bipolar junction transistors. PNP BJT Q


3


may also be replaced with a NPN BJT.




While the present invention has been described herein with reference to particular embodiments thereof, a latitude of modification, various changes and substitutions are intended in the foregoing disclosure, and it will be appreciated that in some instances some features of the invention will be employed without a corresponding use of other features without departing from the scope of the invention as set forth. Therefore, many modifications may be made to adapt a particular situation or material to the teachings of the invention without departing from the essential scope and spirit of the present invention. It is intended that the invention not be limited to the particular embodiments disclosed, but that the invention will include all embodiments and equivalents falling within the scope of the claims.



Claims
  • 1. A band gap reference circuit coupled to a source of bias current, the baud gap reference circuit comprising:an amplifier comprising a differential pair of first and second bipolar junction transistors; a first circuit comprising a first P-N junction coupled to the first bipolar junction transistor; a second circuit comprising a second P-N junction coupled to the second bipolar junction transistor; a first resistor coupled to the first circuit; a second resistor coupled to the first resistor and the second circuit; and a feedback circuit coupled to the amplifier and to the source of bias current, wherein the band gap reference circuit provides an output voltage tat is substantially constant over a range of the bias current.
  • 2. The band gap reference circuit of claim 1 wherein the first and second bipolar junction transistors are PNP transistors.
  • 3. The band gap reference circuit of claim 1 wherein the band gap reference circuit provides an output voltage at the base of the first bipolar junction transistor that is substantially constant over a range of temperatures.
  • 4. The band gap reference circuit of claim 1 wherein:the first P-N junction in the first circuit forms a portion of a third bipolar junction transistor, and the first circuit further comprises a fourth bipolar junction transistor coupled to the third bipolar junction transistor; and the second P-N junction in the second circuit forms a portion of a fifth bipolar junction transistor, and the second circuit further comprises a sixth bipolar junction transistor coupled to the filth bipolar junction transistor.
  • 5. The band gap reference circuit of claim 4 wherein:the first circuit further comprises a seventh bipolar junction transistor coupled to the fourth bipolar junction transistor and the first resistor; and the second circuit further comprises an eighth bipolar junction transistor coupled to the seventh transistor and the second resistor; the third, fourth, and seventh bipolar junction transistors being coupled together as emitter followers; and the fifth, sixth, and eighth transistors being coupled together as emitter followers.
  • 6. The band gap reference circuit of claim 5 wherein the three emitter follower coupled bipolar junction transistors of the first circuit are PNP transistors; and the three emitter follower coupled bipolar junction transistors of the second circuit are PNP transistors.
  • 7. The band gap reference circuit of claim 1 wherein the feedback circuit comprises a third transistor coupled to the amplifier.
  • 8. The band gap reference circuit of claim 7 wherein the feedback circuit comprises a diode coupled sixth fourth bipolar junction transistor coupled to the third transistor.
  • 9. The band gap reference circuit of claim 1 wherein:the first P-N junction in the first circuit faints a portion of a third NPN bipolar junction transistor, and the first circuit further comprises a fourth NPN bipolar junction transistor coupled to the third NPN bipolar junction transistor, and a fifth NPN bipolar junction transistor coupled to the fourth NPN bipolar junction transistor; and the second P-N junction in the second circuit forms a portion of a sixth NPN bipolar junction transistor, and the second circuit further comprises a seventh NPN bipolar junction transistor coupled to the sixth bipolar junction transistor, and an eight NPN bipolar junction transistor coupled to the seventh NPN bipolar junction transistor.
  • 10. The band gap reference circuit of claim 1 wherein the amplifier, the first and second circuits, the first and second resistors, and the feedback circuit all receive at least some of their bias current from the source of bias current.
  • 11. A band gap reference circuit coupled to a source of bias current, the band gap reference circuit comprising:an amplifier comprising a differential pair of first and second bipolar junction transistors; a first circuit comprising third, fourth, and fifth emitter follower coupled bipolar junction transistors; a second circuit comprising sixth, seventh, and eighth emitter follower coupled bipolar junction transistors; a first resistor coupled to the first circuit; a second resistor coupled to the first resistor and the second circuit; and a feedback circuit coupled to the amplifier and to the source of bias current; wherein each of the third, the fourth, and the fifth emitter follower bipolar junction transistors of the first circuit have base-emitter junction areas that are eight times the base-emitter junction areas of each of the sixth, the seventh, and the eighth emitter follower bipolar junction transistors of the second circuit.
  • 12. A band gap reference circuit coupled to a source of bias current, the band gap reference circuit comprising:an amplifier comprising a differential pair of first and second bipolar junction transistors; a first circuit comprising first, second, and third diodes counted in series, the first diode being coupled to the first bipolar junction transistor; a second circuit comprising fourth, fifth, and sixth diodes coupled in series, the fourth diode being coupled to the second bipolar junction transistor; a first resistor coupled to the first circuit; a second resistor coupled to the first resistor and the second circuit; and a feedback circuit coupled to the amplifier and to the source of bias current.
  • 13. A band gap reference circuit coupled to a source of bias current, the band gap reference circuit comprising:an amplifier comprising a differential pair of first and second bipolar junction transistors; a first circuit comprising third and fourth emitter follower coupled bipolar junction transistors, wherein the third bipolar junction transistor is coupled to the first bipolar junction transistor; and the fourth bipolar junction transistor is coupled to a first diode; a second circuit comprising fifth and sixth emitter follower coupled bipolar junction transistors, wherein the fifth bipolar junction transistor is coupled to the second bipolar junction transistor, and the sixth bipolar junction transistor is coupled to a second diode; a first resistor coupled to the first circuit; a second resistor coupled to the first resistor and the second circuit; and a feedback circuit coupled to the amplifier and to the source of bias current.
  • 14. A band gap reference circuit coupled to a source of bias current, the band gap reference circuit comprising:an amplifier comprising a differential pair of first and second bipolar junction transistors; a first circuit comprising a first P-N junction coupled to the first bipolar junction transistor; a second circuit comprising a second P-N junction coupled to the second bipolar junction transistor; a first resistor coupled to the first circuit; a second resistor coupled to the first resistor and the second circuit; and a feedback circuit coupled to the amplifier and to the source of bias current, wherein the first transistor has a base-emitter junction area that is eight times the base-emitter junction area of the second transistor.
  • 15. A method for providing an output reference voltage from a reference circuit coupled to a bias current source, the method comprising:providing the output reference voltage using a first P-N junction and a first resistor; providing a second voltage using a second P-N junction and a second resistor coupled to the first resistor; comparing the output reference voltage to the second voltage using a differential pair comprising first and second bipolar junction transistors; and regulating a first current through a feedback circuit coupled to the differential pair to compensate for variations in a second current through the first and second resistors so that the second current through the first and second resistors remains substantially constant over a range of bias current from the bias current source.
  • 16. The method of claim 15 wherein the differential pair is coupled to a current minor circuit.
  • 17. The method of claim 15 wherein the first P-N junction farina a portion of a third bipolar junction transistor, and the second P-N junction forms a portion of a fourth bipolar junction transistor.
  • 18. The method of claim 15 whereinthe first P-N junction forms a portion of a third bipolar junction transistor, and the output reference voltage is provided using the third, a fourth, and a fifth bipolar junction transistors and the first resistor, and the second P-N junction forms a portion of a sixth bipolar junction transistor, and the second voltage is provided using the sixth, a seventh, and an eighth bipolar junction transistors and the second resistor.
  • 19. The method of claim 18 whereinthe third, the fourth, and the fifth bipolar junction transistors are emitter follower coupled; and the sixth, the seventh, and the eighth bipolar junction transistors are emitter follower coupled.
  • 20. The method of claim 19 wherein each of the third, fourth, and fifth bipolar junction transistors have base-emitter junction areas that are eight times the base-emitter junction areas of each of the sixth, seventh, and eight bipolar junction transistors.
  • 21. The method of claim 15 whereinthe first P-N function is a first diode, the output reference voltage being provided using the first, a second, and a third diodes coupled in series; and the second P-N junction is a fourth diode, the second voltage being provided using the fourth, a fifth, and a sixth diodes coupled in series.
  • 22. The method of claim 15 wherein the output reference voltage is substantially constant over a range of temperature.
  • 23. A method for providing an output reference voltage, the method comprising:providing the output reference voltage using first second, and third diodes coupled in series, and a first resistor; providing a second voltage using fourth, fifth, and sixth diodes coupled in series, and a second resistor that is coupled to the first resistor; comparing the output reference voltage to the second voltage using a differential pair comprising first and second bipolar junction transistors; and regulating a current through a feedback circuit coupled to the differential pair to compensate for variations in current through the first and second resistors.
  • 24. A method for providing an output reference voltage, the method comprising:providing the output reference voltage using a first P-N junction and a first resistor; providing a second voltage using a second P-N junction and a second resistor coupled to the first resistor; comparing the output reference voltage to the second voltage using a differential pair comprising first and second bipolar junction transistors; and regulating a current through a feedback circuit coupled to the differential pair to compensate for variations in current through the first and second resistors; wherein the feedback circuit comprises a MOSFET that regulates its drain-source current.
  • 25. The method of claim 24 wherein the MOSFET is coupled to a diode coupled third bipolar junction transistor.
  • 26. A band gap reference circuit coupled to a source of bias current, the band gap reference circuit comprising:an amplifier comprising a differential pair of first and second bipolar junction transistors; a first resistor; a first circuit comprising a first P-N junction, wherein the first circuit is coupled between the first bipolar junction transistor and the first resistor; a second resistor coupled to the first resistor; a second circuit comprising a second P-N junction, wherein the second circuit is coupled between the second bipolar junction transistor and the second resistor; and a feedback circuit coupled to the amplifier and to the source of bias current.
  • 27. The band gap reference circuit of claim 26 wherein the first P-N junction forms a portion of a third bipolar junction transistor, and the second P-N junction forms a portion of a fourth bipolar junction transistor.
  • 28. The band gap reference circuit of claim 27 wherein the first circuit further comprises a fifth bipolar junction transistor coupled to the third bipolar junction transistor, and a sixth bipolar junction transistor coupled to the fifth bipolar junction transistor, andthe second circuit further comprises a seventh bipolar function transistor coupled to the fourth bipolar junction transistor, and an eighth bipolar junction transistor coupled to the seventh bipolar junction transistor.
CROSS-REFERENCES TO RELATED APPLICATIONS

This application claims priority from U.S. Provisional Patent Application No. 60/220,068, filed Jul. 21, 2000, which is incorporated by reference herein.

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Entry
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Provisional Applications (1)
Number Date Country
60/220068 Jul 2000 US