Curvature correction of bipolar bandgap references

Claim 2

In a solid-state regulated voltage supply of the type including first and second transistors operated at different current densities and connected with associated circuitry to develop a current with a positive temperature coefficient (TC) proportional to the difference in the respective base-to-emitter-voltages of said transistors, said current passing through at least first and second resistors to develop in the first resistor a first corresponding voltage and in the second resistor a second corresponding voltage, the second resistor having a TC that is substantially more positive than the TC of the first resistor, and the second corresponding voltage having a corresponding positive TC substantially exceeding the TC of the first corresponding voltage, the voltage supply including means combining said first and second corresponding voltages with a negative TC voltage derived from the base-to-emitter-voltage of one of the first and second transistors, to provide a composite temperature compensated output voltage, the improvement comprising: the resistance values of the first and second resistors being such as to cause the voltage V comp at the junction of the first and second resistors, at the ambient temperature T o to be described by the formula ##EQU4## where M is the "curvature factor" of V BE for the semiconductor process used to make the transistors; C is the first order temperature coefficient of the material used for the second resistor, referenced from zero degrees Kelvin; and V To 32 kTo/q, where k is the Boltzmann constant and q is the electronic charge.

Claim 3

The bandgap reference circuit of claim 1 wherein the resistance values of the first and second resistors are additionally set so that the output voltage V BG satisfies the relationship V.sub.BG =V.sub.go +V.sub.To (M-1)/2.

Claim 4

In the manufacture of a solid state regulated voltage supply of the type including first and second transistors, first and second resistors connected in series between the emitter of the first transistor and a reference line such that the second resistor is the one connected to the reference line, and a third resistor connected between the emitters of the first and second transistors, means for providing a predetermined nonunity ratio of current densities for the currents passing through the emitters of the first and second transistors, and wherein the second resistor is formed with a temperature coefficient which is substantially more positive than the temperature coefficients of the first and third transistors, the method of compensating for first and second order thermal effects of the difference in base emitter voltages of the first and second transistors comprising the steps of: a. providing the first, second and third resistors with approximate values given by the formulas ##EQU5## where the variables have the following meaning: R a is the resistance of the first resistor; R bo is the resistance of the second resistor at zero degrees Kelvin; R 2 is the resistance of the third resistor; A is the ratio of emitter areas of the first and second transistors; M is the "curvature factor" of V BE for the semiconductor process used to make the transistors; V go is the bandgap voltage using that semiconductor process; C is the first order temperature coefficient of the resistor material used for the second resistor; V To =kTo/q, where k is the Boltzmann constant and q is the electronic charge; and I Co is the value of each collector current at temperature T=To; b. measuring the voltage V comp at the junction of the first and second resistors and trimming the value of the third resistor, R 2 , to adjust the value of V comp to satisfy the relationship ##EQU6## c. measuring the output voltage of the source, V BG and trimming the resistance value of the first resistor, R a , to adjust V BG to satisfy the relationship V.sub.BG =V.sub.go +V.sub.To (M-1)/2.

Claim 5

In the manufacture of a solid state regulated voltage supply of the type including first and second transistors, first and second resistors connected in series between the emitter of the first transistor and a reference line such that the second resistor is the one connected to the reference line, and a third resistor connected between the emitters of the first and second transistors, means for providing a predetermined nonunity ratio of current densities for the currents passing through the emitters of the first and second transistors, and wherein the second resistor is formed with a temperature coefficient which is substantially more positive than the temperature coefficients of the first and third transistors, the method of compensating for first and second order thermal effects of the difference in base emitter voltages of the first and second transistors comprising the steps of: a. providing the first, second and third resistors with approximate values given by the formulas ##EQU5## where the variables have the following meaning: R a is the resistance of the first resistor; R bo is the resistance of the second resistor at zero degrees Kelvin; R 2 is the resistance of the third resistor; A is the ratio of emitter areas of the first and second transistors; M is the "curvature factor" of V BE for the semiconductor process used to make the transistors; V go is the bandgap voltage using that semiconductor process; C is the first order temperature coefficient of the resistor material used for the second resistor; V To =kTo/q, where k is the Boltzmann constant and q is the electronic charge; and I Co is the value of each collector current at temperature T=To; b. measuring the voltage V comp at the junction of the first and second resistors and trimming the value of the third resistor, R 2 , to adjust the value of V comp to satisfy the relationship ##EQU6## c. measuring the output voltage of the source, V BG and trimming the resistance value of the first resistor, R a , to adjust V BG to satisfy the relationship V.sub.BG =V.sub.go +V.sub.To (M-1)/2.

Claim 6

In the manufacture of a solid-state regulated voltage supply of the type including first and second transistors, first and second resistors connected in series between the emitter of the first transistor and a reference line such that the second resistor is the one connected to the reference line, and a third resistor connected between the emitters of the first and second transistors, means for providing a predetermined nonunity ratio of current densities for the currents passing through the emitters of the first and second transistors such that the first transistor operates with a collector current I C1 and the second transistor operates with a collector current I C2 , and wherein the second resistor is formed with a temperature coefficient which is substantially more positive than the temperature coefficients of the first and third transistors, the method of compensating for first and second order thermal effects of the difference in base-emitter voltages of the first and second transistors comprising the steps of: a. providing the first, second and third resistors with approximate values given by the formulas ##EQU7## where the variables have the following meaning: R a is the resistance of the first resistor; R bo is the resistance of the second resistor at zero degrees Kelvin; R 2 is the resistance of the third resistor; A is the ratio of collector currents of the first and second transistors; M is the "curvature factor" of V BE for the semiconductor process used to make the transistors; V go is the bandgap voltage using that semiconductor process; C is the first order temperature coefficient of the resistor material used for the second resistor; V To =kTo/q, where k is the Boltzmann constant and q is the electronic charge; and I Co is the value of each collector current at temperature T=To; b. measuring the voltage V comp at the junction of the first and second resistors and trimming the value of the third resistor, R 2 , to adjust the value of V comp to satisfy the relationship ##EQU8## c. measuring the output voltage of the source, V BG and trimming the resistance value of the first resistor, R a , to adjust V BG to satisfy the relationship V.sub.BG =V.sub.go +V.sub.To (M-1)/2.

Claim 7

In the manufacture of a solid-state regulated voltage supply of the type including first and second transistors, first and second resistors connected in series between the emitter of the first transistor and a reference line such that the second resistor is the one connected to the reference line, and a third resistor connected between the emitters of the first and second transistors, means for providing a predetermined nonunity ratio of current densities for the currents passing through the emitters of the first and second transistors such that the first transistor operates with a collector current I C1 and the second transistor operates with a collector current I C2 , and wherein the second resistor is formed with a temperature coefficient which is substantially more positive than the temperature coefficients of the first and third transistors, the method of compensating for first and second order thermal effects of the difference in base-emitter voltages of the first and second transistors comprising the steps of: a. providing the first, second and third resistors with approximate values given by the formulas ##EQU7## where the variables have the following meaning: R a is the resistance of the first resistor; R bo is the resistance of the second resistor at zero degrees Kelvin; R 2 is the resistance of the third resistor; A is the ratio of collector currents of the first and second transistors; M is the "curvature factor" of V BE for the semiconductor process used to make the transistors; V go is the bandgap voltage using that semiconductor process; C is the first order temperature coefficient of the resistor material used for the second resistor; V To =kTo/q, where k is the Boltzmann constant and q is the electronic charge; and I Co is the value of each collector current at temperature T=To; b. measuring the voltage V comp at the junction of the first and second resistors and trimming the value of the third resistor, R 2 , to adjust the value of V comp to satisfy the relationship ##EQU8## c. measuring the output voltage of the source, V BG and trimming the resistance value of the first resistor, R a , to adjust V BG to satisfy the relationship V.sub.BG =V.sub.go +V.sub.To (M-1)/2.