Note: Descriptions are shown in the official language in which they were submitted.
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A BIAS CURRENT REFERENCE CIRCUIT HAVING A SUBSTANTIALLY
ZERO TEMPERATURE COEFFICIENT
Technical Field
This invention relates generally to reference
circuits and, more particularly, to a circuit for
provlding a current bias source having a near zero
temperature coefficient at a predetermined temperature.
10,
Background Art
A common voltage reference from which bias currents
are established is the ~VBE of two transistors as
taught by Roger Whatley in United States Patent
No. ~,450,367 assigned to the assignee hereof entitled
" ~VBE Bias Current Reference Circuit". As noted by
Whatley, the ~VBE voltage has a known positive
temperature coefEicient. A resistor which is utilized to
provide a reference current also has a known positive
temperature coefficient. Although a ~VBE bias current
reference circuit exhibits a lower temperature coefficient
than a VBE bias current reference circuit, the
temperature coefficient of the ~VBE cixcuit is
determined by the temperature coefficient of resistors and
is nonzero.
Summary of the Invention
It is an object of the present invention to provide
an improved bias current reference circuit.
Another object of the present invention is to provide
an improved bias current reference circuit having a
substantially zero temperature coefficient.
In carrying out the above and other objects of the
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present invention, there is provided, in one form, a bias
current reference circuit which has a substantially zero
temperature coefficient. A reference voltage portion
comprising a first bipolar transistor provides a reference
voltage which is proportional to a bias current. A
reference current portion is coupled to the reference
voltage portion and comprises a second bipolar transistor
and first and second resistors having first and second
predetermined temperature coefficients, respectively. The
difference in the base to emitter voltages, ~VBE, has
a third predetermined temperature coefficient. The
reference current portion provides a reference current
which is proportional to ~VBE and the resistance of
the first and second resistors. A weighted sum of the
first and second temperature coefficients is made
substantially equal to the third temperature coefficient.
A bias voltage portion is coupled to the reference current
portion and provides a bias voltage proportional to the
reference current to both a bias current portion and an
output portion. The output portion provides an output
bias current in response to an attached load.
The above and other objects, features and advantages
of the present invention will be more clearly understood
from the following detailed description taken in
conjunction with the following drawings.
Brief Description of tne Drawing
The single Figure illustrates in schematic form a
bias current reference circuit in accordance with the
present invention.
Detailed Description of the Present Invention
Shown in the single Figure is a bias current
.
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reference circuit 10 generally comprising a reference
voltage portion 11, a reference current portion 12, a bias
voltage portion 13, a bias current portion 1~ and an
output portion 15. Although specific N-channel and
P-channel MOS transistors and bipolar transistors are
illustrated, it should be apparent that bias current
reference circuit 10 could be implemented by completely
reversing the processing techniques (e.g. P-channel to
N-channel) or by using other types of transistors.
Reference voltage portion 11 comprises a bipolar NPN
transistor 16 having a collector and a base connected
together at a terminal for receiving a first supply
voltage VDD. In a preferred form, supply voltage
VDD is positive. An emitter of transistor 16 is
connected to a source of a P-channel transistor 17.
Transistor 17 is diode-configured by connecting its gate
to a drain thereof.
Reference current portion 12 comprises a bipolar NPN
transistor having a collector and a base connected togther
at the terminal for receiving supply voltage VDD. An
emltter of transistor 20 is connected to a first terminal
of a resistor 21. A second terminal of resistor 21 is
connected to a first terminal of a resistor 22. A second
terminal of resistor 22 is connected to a source of a
P-channel transistor 24. A gate of transistor 24 is
connected to the gate of transistor 17.
Bias voltage portion 13 comprises an N-channel
transistor 26 having a drain connected to a drain of
transistor 24. A gate of transistor 26 is connected to
the drain of transistor 26 for providing an output bias
current. A source of transistor 26 is connected to a
second supply voltage Vss. In a preferred form,
supply voltage Vss is the most negative supply
voltage.
Bias current portion 14 comprises an N-channel
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transistor 28 having a drain connected to the drain of
transistor 17. A gate of transistor 28 is connected to
the ga~e of transistor 26. A source of transistor 28 is
connected to supply voltage Vss.
Output portion 15 comprises an N-channel transistor
2~ having a gate connected to the drains of transistors 24
and 26. A source of transistGr 29 is connected to supply
voltage Vss and a drain of transistor 29 provides an
output terminal 30. An output load 31 has a first
terminal coupled to outpu~ terminal 30 and a second
terminal connected to supply voltage VDD.
In operation, transistor 16 develops a first VBE
voltage across its base-to-emitter electrodes, and
transistor 20 develops a second VBE voltage across its
current electrodes. A ~VB~ voltage is developed
across resistors 21 and 22 which provides a reference bias
current, say I1, through transistors 24 and 26.
Transistor 24 is constructed with a channel width to
channel length ratio such that transistors 17 and 24 have
the same channel .current density. Therefore, the
gate-source voltage of transistor 24 is substantially
equal to the gate-source voltage of transistor 17.
Applying Kirchoff's voltage law to the loop comprising
transistors 16, 17, 20 and 24 and resistors 21 and 22,
results in the equation:
VBE16 - VgE20 ~ ~VBE
where VBE16 and VBE20 represent the base to
emitter voltages of transistors 16 and 20, respectively,
and avBE is the d.ifference in the base--to-emitter
voltages whlch will be reflected across resistors 21 and
22. Transistor 26 provides a bias voltage equal to its
gate-to-source voltage, VGs, and proportional to the
35 reference current I1. Transistors 26 and 28 are ratioed
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to mirror a proportional current through transistor 2~.
Similarly, transistors 26 and 29 are ratioed so that
transistor 26 mirrors a current proportional to the
reference current through transistor 29. Transistor 29
provides an output current when coupled to an external
load such as load 31.
The illustrated embodiment differs from prior art
circuits in that the resistance used in reference current
portion 12 is implemented as two distinct or separate
resistors having differing temperature coefficients to
provide a bias current reference circuit having a
substantially zero temperature coefficient. The bias
current I1 can be expressed as:
I1 = (~\VBE) / (R21 + R22)
where it can be readily shown that
V3E=[(kT)/(q)]xln[I16/I2o)x(A2o/A16)]
where, k = Boltzman's constant;
T = temperature in degrees Centigrade;
q = electrical. charge in Coulombs;
I16 = the current in Amperes through transistor 16;
I20 = the current in Amperes through transistor 20;
A20 = the emitter junction area of transistor 20; and
A16 = the emitter junction area of transistor 16.
The conventionally known temperature coefficient of
AVBE is approximately +3400 ppm/-C. In order for bias
current I1 to have a zero temperature coefficient, the
following equation must be satisfied:
d/dT (I1) = 0.
From the above equations/ it can be readily shown that the
temperature coefficient of bias current I1 equals the
ratio of the combined temperature coefficient of resistors
21 and 22 and ~VBE at a predetermined temperature.
Therefore, if the combined temperature coefficient of
resistors 21 and 22 is approximately +3400 ppm/~C, a
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substantially zero temperature coefficient results. This
combined temperature coefficient should also be positive
rather than having both positive and negative temperature
coefficients since the temperature coefficient of I1 is
a ratio. Unfortunately, a single resistive component
having a temperature coefficient of +3400 ppm/~C is
typically not fabricated in any conventional electronic
process. However, there are numerous processes such as
MOS in which resistive components having positive
temperature coefficients of much greater and much less
than ~3400 ppm/C are both fabricated on the same
integrated circuit. Therefore, a resistor having a
composite temperature coefficient of approximately +3400
ppm/GC can be fabricated by taking a weighted sum value of
resistors 21 and 22 wherein resistor 21 may have a
temperature coefficient greater than +3~00 ppm/~C and
resistor 22 may have a temperature coefficient less than
-~3400 ppm/C. Resistors 21 and 22 are size ratioed with
respect to aach other so that the effective temperature
coefficient is +3400 ppm/CC, a temperature coefficient
normally not available in conventional MOS processes. In
a preferred form, resistors 21 and 22 are fabricated as P-
and P+ resistors, respectively. By using P- and P+
resistors, an ohmic contact which does not require
metalization may be fabricated between the two composite
resistors. Metal contacts have a very inaccurate and
variable impedance associated therewith and the avoidance
of metal contacts is desirable for precise ternperature
coefficient accuracy. Within some CMOS processes,
resistor 21 may be fabricated as a P- resistor from a tub
diffusion and resistor 22 may be fabricated as a P~
resistor from a source-drain diffusion. Within any CMOS
process, when semiconductor tubs are very lightly doped,
resistors having high temperature coefficients result.
Therefore, resistor 21 may be fabricated having a known high
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temperature coefficient for predetermined dimensions.
Since resistor 22 is a P~ resistor which is very heavily
doped, a low temperature coefficient in the range of
1000-1500 ppm/iC results. By using P- and P~ resistors,
less space is required than other types of equal valued
resistors because of the high sheet rho of P-. Increased
absolute accuracy is obtained due to the smaller initial
tolerance of P+ than P-.
Additionally, P+ or N~ poly resistors having
different temperature coefficients may be used to provide
a bias current reference circuit having a near zero
temperature coefficient. Although specific types of
reæistors have been discussed, other types of resistors
may be used. The method of the invention is to use a
first resistor having a temperature coefficient greater
than a ~VBE temperature coefficient and a second
resistor having a temperature coefficient less than a
~VBE temperature coefficient. The first and second
resistors are then ratioed to provide a composite resistor
equal to the ~VgE temperature coefficient.
By now it should be understood that a bias current
reference circuit having a near zero temperature
coefficient has been provided. By ratioing two resistors
having known different temperature coefficients, an
effective resistance with a desired temperature
coefficient required to provide a near zero circuit
temperature coefficient results. Therefore, a bias
current reference circuit having minimal temperature
dependence is provi~ed without increasing circuit
complexity.
While the invention has been described in the context
of a preferred embodiment, it will be apparent to those
skilled in the art that the present invention may be
modified in numerous ways and may assume many embodiments
other than that specifically set out and described above.
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Accordingly/ it is intended by the appended claims to
cover all modifications of the invention which fall within
the true spirit and scope of the invention.