This invention relates to a CMOS reference voltage circuit and, more particularly, to a CMOS reference voltage circuit formed on a semiconductor integrated circuit, the CMOS reference voltage circuit having a small chip area, operating from low voltage and exhibiting a temperature characteristic that is small.
A conventional CMOS reference voltage circuit is described in detail in the specification of Japanese Patent Kokai Publication No. JP-A-11-45125. In terms of obtaining a reference voltage by a current-to-voltage conversion, this reference voltage circuit naturally is the same as an earlier devised reference voltage circuit of this kind in which a temperature characteristic is cancelled out. However, in the earlier devised reference voltage circuit in which the temperature characteristic is cancelled out, a reference current having a positive temperature characteristic is converted to a voltage by a circuit comprising a resistor and a diode (or a diode-connected transistor), and the circuit obtains a voltage component in which the amount of voltage drop at the resistor has a positive temperature characteristic and a voltage component in which the forward voltage at the diode (or diode-connected transistor) has a negative temperature characteristic, and adds these temperature characteristics, thereby obtaining a reference voltage of about 1.2V in which the temperature characteristic has been cancelled out.
On the other hand, with the proposed reference voltage circuit described in the above-cited Japanese Patent Kokai Publication No. JP-A-11-45125, a reference current having almost no temperature characteristic is obtained, the current is converted to a voltage by an output circuit comprising only a resistor, and a reference voltage having any desired voltage value is obtained.
Accordingly, since 1.2V, from which the temperature characteristic has been cancelled out, stipulated as the output voltage of this conventional type of reference voltage circuit is obtained upon being converted to a current value within the circuit, the reference voltage circuit is outstanding in that in can be operated at a power-supply voltage of less than 1.2V.
In the textbook entitled “Analog Circuit Design Techniques for Applying CMOS to Mobile Wireless Terminals” (1999, published by Torikeppsu K.K.), the author of which is the present Inventor, a “Current-Mode-Type Reference Voltage Circuit” that was made public immediately within the same year is introduced and a detailed circuit analysis thereof is described.
In particular, in reference voltage circuits thus far, since use is made of a forward voltage of a diode (or diode-connected transistor) and this is a voltage component having a negative characteristic, a deviation from the temperature characteristic regarding the forward voltage of the diode (or diode-connected transistor) appears in the output voltage to a marked extent.
That is, although the forward voltage of the diode (or diode-connected transistor) possesses a negative temperature characteristic, the slope of the negative temperature characteristic becomes blunt as temperature falls.
On the other hand, a voltage having a positive characteristic is realized by obtaining a current, which flows into a resistor, owing to a difference voltage between forward voltages of two diodes (or diode-connected transistors) having different current densities, and converting this current to a voltage by the resistor.
In accordance with the content described in the patent document cited above, the operation thereof will be described. As shown in
Accordingly, we have
VA′=VB′ (1)
Further, currents I1, I2 that are output from p-channel MOS transistors P1, P2, respectively, are equal to each other.
I1=I2 (2)
The current I1 is split into a current I1A that flows into a diode D1 and a current I1B that flows into a resistor R4 (=R4A+R4B). Similarly, the current I2 is split into a current I2A that flows into a serially connected resistor R1 and commonly into N-number of parallel-connected diodes D2, and a current I2B that flows into a resistor R2 (=R2A+R2B).
If we assume the following:
R2=R4 (3)
then Equations (4) and (5) below will hold.
I1A=I2A (4)
I1B=I2B (5)
Accordingly, we have the following:
VA=VB (6)
Further, if we assume that the forward voltages of diodes D1 and D2 are VF1 and VF2, respectively, then replacing, we have the following:.
VA=VF1 (7)
VB=VF2+ΔVF (8)
From Equations (7) and (8), we have the following:
ΔVF=VF1−VF2 (9)
The voltage drop across the resistor R1 is ΔVF, and the currents I2A and I1B are represented by Equations (10), (11), respectively, below.
I2A=ΔVF/R1 (10)
I1B=I2B=VF1/R2 (1)
Here the following holds:
ΔVF=VT1n(N) (12)
where VT represents thermal voltage and is expressed by
VT=kT/q (13)
where T represents absolute temperature [K], k the Boltzmann constant and q the unit electronic charge.
An output current 13 (=I2) of a p-channel MOS transistor P3 is converted to a voltage by a resistor R3, and an output voltage Vref is expressed by Equation (14) below.
In Equation (14), {VF1+(R2/R1)[VT1n(N)]} is a voltage value of about 1.205V from which the temperature characteristic has been cancelled. More specifically, VF1 has a negative temperature characteristic (temperature coefficient) of about −1.9 mV/° C., and VT has a positive temperature characteristic (temperature coefficient) of 0.0853 mV/° C. Accordingly, the temperature characteristic of the output voltage Vref is cancelled out, and therefore the value of (R2/R1)1n(N) is 22.27.
Further, since VT is 26 mV at an ambient temperature, (R2/R1)[VT1n(N)] is approximately 579 mV at an ambient temperature. Accordingly, if we assume that VF1 is 626 mV at an ambient temperature, then {VF1+(R2/R1)[VT1n(N)]} will be approximately 1.205V.
The temperature characteristic will now be discussed in detail. A resistor R4 is connected in parallel with the diode D1. If the temperature is low, therefore, the value of the current I1B that flows into the resistor R4 (=R4A+R4B) tends to decrease owing to the non-linearity of the temperature characteristic possessed by the diode. On the other hand, a resistor R1 is connected in series with the diode D2. If the current I2A that flows into the diode D2 has a positive temperature characteristic, therefore, then the voltage VB across the diode D2 and resistor R1 will fall below the voltage VA (=VF1) at the diode D1.
Owing to control by the operational amplifier DA1, the two voltages (the voltage VA at diode D1 and the voltage VB across diode D2 and resistor R1) become equal. With an increase in current (the current I2A that flows into the diode D2) at a low temperature, therefore, the two voltages become equal. At a high temperature, on the other hand, the action is the reverse.
That is, in the circuit shown in
Thus, since the drive currents I1, I2 and I3 that are supplied from the p-channel MOS transistors P1, P2 and P3 act in a direction that cancels out the non-linearity of the temperature characteristic exhibited by the forward voltage of the diodes, the temperature characteristic of the reference voltage obtained can also be set to a characteristic that is very near a straight line having little fluctuation with respect to temperature.
Further, since the ratio of the resistors (R3/R2) does not possess a temperature characteristic, the reference voltage Vref that is output also is a voltage from which the temperature characteristic has been cancelled out. Here the resistor ratio (R3/R2) can be set at will.
If I<(R3/R2) is set, the output voltage Vref becomes a voltage higher than 1.205 V, and if I>(R3/R2) is set, the output voltage Vref becomes a voltage lower than 1.205 V
In the above-cited patent document, N=10 is described as the specific value of N. When the circuit is actually implemented [IEEE Symposium on VLSI Circuits (May)], however, N=100 holds.
In the CMOS process, the progress of finer patterning has resulted in MOS transistors of very small size. By contrast, the size of diodes that employ parasitic bipolar elements is greater than that of MOS transistors by an order of magnitude.
Further, since the ratio N between the diodes D1 and D2 in
Japanese Patent Kokai Publication No. JP-A-11-45125
The circuit described in the above-cited patent document has the problems set forth below.
The first problem is an increase in a chip area. The reason is that the diode constituted by a parasitic transistor has a large area.
The second problem is a large variation. The reason is that although temperature dependence is decided predominantly by a p-channel MOS transistor that constitute a current mirror circuit and a diode, the p-channel MOS transistor and diode each vary individually.
In view of the problems set forth above, the present invention seeks to implement a reference voltage circuit that can use a p-channel MOS transistor for a diode, thereby realizing a reference voltage circuit of small chip area that operates from a low voltage and outputs any desired reference voltage exhibiting only a small temperature characteristic. Further, by adopting the same circuit topology for two current-to-voltage converting circuits for being compared and an output current-to-voltage converting circuit, a reference voltage circuit that is little affected by element variations is achieved.
The present invention provides a reference voltage circuit comprising: first and second current-to-voltage converting circuits; control means for exercising control in such a manner that a prescribed output voltage of the first current-to-voltage converting circuit and a prescribed output voltage of the second current-to-voltage converting circuit will become equal; a first current mirror circuit, which has a non-linear input/output characteristic, for supplying current to each of the first and second current-to-voltage converting circuits; a second current mirror circuit, which has a linear input/output characteristic, for outputting a current that is proportional to the value of the current supplied to the first current-to-voltage converting circuit; and a third current mirror circuit, which has a linear input/output characteristic, for outputting a current that is proportional to the value of the current supplied to the second current-to-voltage converting circuit; wherein output current from the second current mirror circuit and output current from the third current mirror circuit are added and the resultant current is converted to voltage via a third current-to-voltage converting circuit and the voltage is supplied.
In the present invention, it is preferred that the third current-to-voltage converting circuit comprise a resistor.
In the present invention, it is preferred that the first and second current-to-voltage converting circuits each include a diode-connected MOS transistor and a voltage-dividing resistor connected in parallel with the MOS transistor; wherein divided voltages from the voltage-dividing resistors of respective ones of the first and second current-to-voltage converting circuits are output as the prescribed output voltages of respective ones of the first and second current-to-voltage converting circuits.
In the present invention, the first current-to-voltage converting circuit has a diode and a voltage-dividing resistor connected in parallel with the diode, and the second current-to-voltage converting circuit has a series circuit, which comprises one diode or a plurality of parallel-connected diodes and a resistor, and a voltage-dividing resistor connected in parallel with the series circuit; wherein divided voltages from the voltage-dividing resistors of respective ones of the first and second current-to-voltage converting circuits are output as the prescribed output voltages of respective ones of the first and second current-to-voltage converting circuits. In the present invention, the diode may be a diode-connected bipolar junction transistor (BJT).
In the present invention, the control means includes a differential amplifying circuit having differential input terminals for receiving respective ones of the prescribed output voltage of the first current-to-voltage converting circuit and the prescribed output voltage of the second current-to-voltage converting circuit, and an output terminal for delivering a voltage that controls a common node of the first to third current mirror circuits.
In the present invention, a diode-connected MOS transistor and a resistor are connected in parallel and a divided voltage is adopted as a voltage to be controlled, thereby lowering the input voltage of a differential amplifying circuit (operational amplifier) and facilitating the implementation of low-voltage operation. Furthermore, in an embodiment of the present invention, there is obtained a reference voltage circuit in which a temperature characteristic is cancelled and which operates from low voltages by setting the output reference voltage set to a low, constant voltage of not more than 1.0V. By constituting the circuit using two diode-connected MOS transistors, the circuit can be implemented with a small chip area.
The meritorious effects of the present invention are summarized as follows.
In accordance with the present invention, it is possible to reduce chip area. The reason for this is that in the present invention, a reference voltage circuit in which the temperature characteristic has been cancelled out can be implemented by MOS transistors without relying upon diodes. In particular, a reference voltage circuit in which the temperature characteristic has been cancelled can be implemented without using parasitic bipolar junction transistors. This contributes to a decrease in chip area.
In accordance with the present invention, the circuit can be operated at low voltages. The reason for this is that in the present invention, the output voltage (reference voltage) can be made any voltage value of 1.0V or less.
In accordance with the present invention, the effects of variation can be reduced. The reason for this is that in the present invention, the circuit is implemented using only MOS transistors and resistors, which are circuit elements, other than those of the differential amplifying circuit (differential amplifier), that predominantly decide the temperature characteristic.
Still other features and advantages of the present invention will become readily apparent to those skilled in this art from the following detailed description in conjunction with the accompanying drawings wherein embodiments of the invention are shown and described, simply by way of illustration of the mode contemplated of carrying out this invention. As will be realized, the invention is capable of other and different embodiments, and its several details are capable of modifications in various obvious respects, all without departing from the invention. Accordingly, the drawing and description are to be regarded as illustrative in nature, and not as restrictive.
The present invention will now be described in detail with reference to the drawings. The present invention includes first to third current-to-voltage converting circuits (101, 102 and 103), first to fourth MOS transistors (M1, M2, M3 and M4) having their gates coupled together, and a differential amplifying circuit (or operational amplifier) (AP1). The first current-to-voltage converting circuit (101) preferably includes a diode-connected fifth MOS transistor (namely a MOS transistor having a coupled drain and gate) (M5) and first voltage-dividing resistors (R2 and R3) connected in parallel with the fifth MOS transistor (M5). The second current-to-voltage converting circuit (102) preferably includes a diode-connected sixth MOS transistor (M6) and second voltage-dividing resistors (R4 and R5) connected in parallel with the second MOS transistor (M6). The third current-to-voltage converting circuit (103) comprises a resistor (R7). The sources of the first and third MOS transistors (M1 and M3) are connected to a power supply (VDD) via resistors (R1 and R6), respectively. The sources of the second and fourth MOS transistors (M2 and M4) are connected to the power supply (VDD), directly. The drains of the first and second MOS transistors (M1 and M2) are connected to the sources of the fifth and sixth MOS transistors (M5 and M6), respectively, of the first and second current-to-voltage converting circuits (101 and 102), respectively. First and second divided voltages (VA and VB) obtained by the first and second voltage-dividing resistors of the first and second current-to-voltage converting circuits (101 and 102), respectively, are applied to an inverting input terminal (−) and non-inverting input terminal (+) of the differential amplifying circuit (AP1). The output terminal of the differential amplifying circuit (AP1) is connected to the coupled gates of the first to fourth MOS transistors (M1, M2, M3 and M4). The first and second MOS transistors (M1 and M2) constitute a current mirror having a non-linear input/output characteristic, and first and third MOS transistors (M1 and M3) constitute a current mirror having a linear input/output characteristic, and the second and fourth MOS transistors (M2 and M4) constitute a current mirror having a linear input/output characteristic. The drains of the third and fourth MOS transistors (M3 and M4) are coupled together and connected to the resistor (R7) of the third current-to-voltage converting circuit (103). An output voltage (VREF) is delivered from the node at which the resistor (R7) of the third current-to-voltage converting circuit (103) is connected to the coupled drains of the third and fourth MOS transistor (M3 and M4).
Alternatively, according to the present invention, the first current-to-voltage converting circuit (101) includes a first diode (D1) having its cathode connected to ground, and first voltage-dividing resistors (R2 and R3) connected in parallel with the diode (D1). The second current-to-voltage converting circuit (102) includes a series circuit comprising a plurality of diodes (D2) having their cathodes connected to ground and their anodes coupled together and a resistor (R0) having a first end connected to the common node of the plurality of diodes (D2), and second voltage-dividing resistors (R4 and R5) connected in parallel with the series circuit. The third current-to-voltage converting circuit (103) comprises the resistor (R7) having a first end connected to ground. The drain of the first MOS transistor (M1) is connected to the anode of the diode (D1) of the first current-to-voltage converting circuit (101). The drain of the second MOS transistor (M2) is connected to the second end of resistor (R0) of the second current-to-voltage converting circuit (102).
In accordance with this embodiment, characteristics and performance can be improved. For example, any output voltage equal to or greater than 1V or less than 1V is obtained. Further, a high precision is obtained. That is, the effects of element variation are alleviated and so are the effects of non-linear temperature characteristics of diodes. Furthermore, it is possible to achieve lower voltage. That is, by making output voltage lower than 1V, operation is possible from about 1.2V. The details of circuitry and operation of the present invention will now be described in detail.
For example, in a self-bias circuit often seen in reference voltage circuits of this kind, there are two operating points. It is well known in the art that it is necessary to add on a so-called start-up circuit in such a manner that the operating point of the circuit will not migrate to an operating point that prevails in a case where there is no flow of current in the circuit.
In
The p-channel MOS transistor M1 and a p-channel MOS transistor M3 form a linear current mirror circuit constituting a second current mirror circuit. The voltage at the coupled gates of these transistors is similarly controlled by the operational amplifier AP1.
Similarly, the p-channel MOS transistor M2 and a p-channel MOS transistor M4 form a linear current mirror circuit constituting a third current mirror circuit, and the voltage at the coupled gates of these transistors is controlled by the operational amplifier AP1.
The output currents from the second and third current mirror circuits (the drain currents of the MOS transistors M3 and M4) are each weighted, and currents flow into the third current-to-voltage converting circuit 103 via the MOS transistors M1 and M2 and are converted to a desired reference voltage VREF.
What is noteworthy here is the temperature characteristic of the non-linear current mirror circuit constituting the first current mirror circuit. In such a non-linear current mirror circuit referred to as a Widlar current mirror circuit, the output current (drain current I1 of the MOS transistor M1) has a positive temperature characteristic with respect to the input reference current (drain current I2 of the MOS transistor M2).
That is, the currents I1 and I2 that flow respectively into the MOS transistors M1 and M2 constituting the first current mirror circuit have temperature characteristics that are different each other. The circuit has a temperature characteristic. Accordingly, the circuit may be considered to have a positive or negative temperature characteristic regardless of whether the temperature characteristic is large or small.
Accordingly, in a case where the prescribed output voltages of the first and second current-to-voltage converting circuits 101 and 102 become equal, there is a possibility that if the current that flows into the second current-to-voltage converting circuit 102 can be set to have a somewhat negative temperature characteristic, then the current that flows into the first current-to-voltage converting circuit 101 can be set to cancel out this negative temperature characteristic and have a somewhat positive temperature characteristic. In this case, it is possible for a reference voltage, which is obtained upon canceling out temperature characteristics by weighting and adding the current having the negative temperature characteristic that flows into the second current-to-voltage converting circuit 102 and the current having the positive temperature characteristic that flows into the first current-to-voltage converting circuit 101, to be set in such a manner that it will have almost no temperature characteristic. This will be described with respect to specific examples.
As shown in
P-channel MOS transistors M1 and M3 form a linear current mirror circuit constituting a second current mirror circuit. The voltage at the coupled gates of these transistors M1 and M3 is similarly controlled by the output of the operational amplifier AP1.
Similarly, p-channel MOS transistors M2 and M4 form a linear current mirror circuit constituting a third current mirror circuit, and the voltage at the coupled gates of these transistors M2 and M4 is controlled by the output of the operational amplifier AP1.
In the implementation shown in
The output currents from the second and third current mirror circuits (the drain currents of the MOS transistors M3 and M4) are each weighted, and currents flow into the third current-to-voltage converting circuit, which comprises resistor R7, via the MOS transistors M1 and M2 and are converted to the desired reference voltage VREF.
In
In a circuit of this kind, describing operation by performing circuit analysis is difficult. The circuit conditions will be enumerated. Since VA=VB holds, Equation (15) below holds.
If we assume that the gate W/L's of the MOS transistors M5 and M6 are K5 and K6 times, respectively, that of a unit MOS transistor (transistor M2 in
K5β(VGS5−VTH)2=I1A (16)
K6β(VGS6−VTH)2=I2A (17)
With regard to currents I1 and I2 that are output from the non-linear current mirror circuit (M1 and M2), the current I1 is split into current I1B that flows into the voltage-dividing resistors R2 and R3 and current I1A that flows into the diode-connected MOS transistor M5, and the current I2 is split into current I2B that flows into the voltage-dividing resistors R4 and R5 and current I2A that flows into the diode-connected MOS transistor M6. Accordingly, the currents I1, I2 are represented by Equations (18) and (19) below.
I1=I1A+I1B (18)
I2=I2A+I2B (19)
Substituting Equations (16) and (17) and I1B=VGS5/(R2+R3), I2B=VGS6/(R4+R5), Equations (18) and (19) become Equations (20) and (21) below.
Solving Equations (20) and (21), Equations (22) and (23) below hold.
Substituting Equations (22) and (23) into Equation (15), we have Equation (24) below.
Here it will suffice if currents I1 and I2 and parameters β, R2, R3, R4, R5, VTH, K5 and K6 for which Equation (24) holds exists.
In particular, the threshold voltage VTH has a negative temperature characteristic, and the transconductance parameter β is a parameter that is proportional to a mobility μ and has a negative temperature characteristic. If this is illustrated in concrete form, the result is as shown in
Further, since the MOS transistor M1 in which the source resistor R1 has been inserted and the MOS transistor M2 having no source resistor form a non-linear current mirror circuit, specifically a Widlar current mirror circuit, the currents I1 and I2 that flow into the MOS transistors M1 and M2, respectively, are represented by Equations (25) and (26) below, in which MOS transistor M2 serves as a unit MOS transistor.
K1β(VGS1−VTH)2 =I1 (25)
β(VGS2−VTH)2 =I2 (26)
Further, since the gates of the MOS transistor M1 and MOS transistor M2 are coupled together, the sum of the gate-to-source voltage VGS1 of MOS transistor M1 and terminal voltage R1I1 of resistor R1 becomes the gate-to-source voltage VGS2 of the MOS transistor M2 and satisfies Equation (27) below.
VGS2=VGS1+R1I1 (27)
Substituting Equation (27) into Equations (25) and (26) and solving, we have the following:
Equation (28) illustrates the input/output characteristic of the well-known Widlar current mirror circuit. It should be noted that this equation is not indicated by a function of type I1=f(I2) but by the inverse function, namely I2=f(I1). If illustrated, the result is as shown in
Thus, it will be understood that if the temperature characteristics become the opposite of each other, such as the temperature characteristic of current I1 being positive and the temperature characteristic of current I2 being negative, then the divided output voltage VA of the first current-to-voltage converting circuit and the divided output voltage VB of the second current-to-voltage converting circuit in
What is noteworthy here is that the voltage-dividing resistor ratios R3(R2+R3) and R5/(R4+R5) in Equation (15) are constant values that do not possess a temperature characteristic.
By contrast, even if the temperature characteristics of the resistors is neglected, the gate-to-source voltages VGS5 and VGS6 of the p-channel MOS transistors M5 and M6 are governed by temperature characteristics possessed by the parameters β and VTH.
Accordingly, in a self-biased linear current mirror circuit, even if the first current-to-voltage converting circuit 101 and second current-to-voltage converting circuit 102 are driven by mutually proportional currents whose temperature characteristics are equal so that the divided output voltage VA of the first current-to-voltage converting circuit 101 and the divided output voltage VB of the second current-to-voltage converting circuit 102 are made to agree, naturally the temperature characteristics of the two drive currents will agree and will be positive temperature characteristics. However, if drive is performed by a non-linear current mirror circuit, as in the present invention, it will be unnecessary for the two currents to be proportional. The operating point is therefore decided with a degree of freedom and a difference will occur also in the temperature characteristics between the driving currents.
A Widlar current mirror circuit, which is a non-linear current mirror circuit, has a positive temperature characteristic inherently. It is also possible, therefore, to set the temperature characteristic of one current to negative and set the temperature characteristic of the other current to positive.
It goes without saying that the diode-connected MOS transistors of the first and second current-to-voltage converting circuits can be changed to diode-connected bipolar transistors or diodes, as illustrated in
In order that the operating point will be decided in the second current-to-voltage converting circuit, the number of diode-connected bipolar transistors or diodes is made N and a resistor R0 is added. In the implementation of
Various reference voltage circuits integrated on an LSI chip can be mentioned as an example of use of the present invention. In particular, recent advances in terms of the formation of ever finer patterns in IC processes have been accompanied by a reduction in the power-supply voltage supplied to LSI circuits and there is now need for stable reference voltage circuits that are free of temperature fluctuation and that operate at power-supply voltages of about 1V. The present invention satisfies this need.
As many apparently widely different embodiments of the present invention can be made without departing from the spirit and scope thereof, it is to be understood that the invention is not limited to the specific embodiments thereof except as defined in the appended claims.
It should be noted that other objects, features and aspects of the present invention will become apparent in the entire disclosure and that modifications may be done without departing the gist and scope of the present invention as disclosed herein and claimed as appended herewith.
Also it should be noted that any combination of the disclosed and/or claimed elements, matters and/or items may fall under the modifications aforementioned.
Number | Date | Country | Kind |
---|---|---|---|
2006-020995 | Jan 2006 | JP | national |
Number | Name | Date | Kind |
---|---|---|---|
5625281 | Lambert | Apr 1997 | A |
5977759 | Sitch | Nov 1999 | A |
6160391 | Banba | Dec 2000 | A |
6407619 | Tanaka | Jun 2002 | B1 |
6452437 | Takeuchi et al. | Sep 2002 | B1 |
6903601 | Aude | Jun 2005 | B1 |
Number | Date | Country |
---|---|---|
11-45125 | Feb 1999 | JP |
Number | Date | Country | |
---|---|---|---|
20070176590 A1 | Aug 2007 | US |