Preferred embodiments of the present invention will now be described with reference to the drawings. Note that in each of the following embodiments, elements that are functionally similar to those of any preceding embodiments will be denoted by like reference numerals, and will not be described repeatedly.
Referring to
The BGR-type current generation circuit 100 includes a reference current generation circuit 101 and a current mirror circuit 102.
The reference current generation circuit 101 includes a resistive element 105, and PMOS transistors 106 and 107 (the reference current MOS transistors) whose transistor size ratio is 1:M.
The current mirror circuit 102 includes NMOS transistors 108 and 109 (the current mirror MOS transistors). The NMOS transistors 108 and 109 are designed so that an equal source-drain current flows therethrough by, for example, using the same transistor size.
The resistive load circuit 103 includes a PMOS transistor 110 (the load section MOS transistor) whose gate and drain are connected to each other (diode connection), and a resistive element 111.
The node at which the BGR-type current generation circuit 100 and the resistive load circuit 103 are connected to each other is referred to as a node 114 (the second node), and the voltage at the node 114 is denoted as Va.
The reference voltage output stage 104 includes an NMOS transistor 112 and a PMOS transistor 113 (the output stage MOS transistor), and outputs the voltage at a node 115 (the output node) as the output voltage Vref (the reference voltage).
The NMOS transistor 109 and the NMOS transistor 112, together forming a current mirror circuit, are designed so that the source-drain current ratio therebetween is 1:2N. The PMOS transistor 110 and the PMOS transistor 113, together forming a current mirror circuit, are designed so that the source-drain current ratio therebetween is 1:N.
The resistance values R1 and R2 of the resistive elements 105 and 111 and the value M in the transistor size ratio 1:M between the PMOS transistors 106 and 107 are determined so that there are little variations in the output voltage Vref with respect to variations in the temperature. How these values are determined in the present invention will now be described in detail.
It is assumed herein that the PMOS transistors 106 and 107 are operating in a sub-threshold region where the gate-source voltage is less than the threshold voltage. Where the gate-source voltage of the PMOS transistor 106 is denoted as Vgsp1, the current I1 flowing through the PMOS transistor 106 can be expressed as shown in Expression 1 below.
In Expression 1, n is a constant dictated by the process, which typically is little dependent on the temperature and takes a value of about 1.4, for example. Isub0 is a constant dictated by the process, which varies with a strong positive temperature gradient with respect to variations in the temperature. W denotes the gate width of the PMOS transistor 106, L the gate length of the PMOS transistor 106, k the Boltzmann constant, T the absolute temperature, and q the charge of electron.
Where the gate-source voltage of the PMOS transistor 107 is denoted as Vgsp2, since an equal current flows through the NMOS transistors 108 and 109, the current I2 flowing through the PMOS transistor 107 is equal to I1, which is expressed as shown in Expression 2 below.
Since the gate voltage of the PMOS transistor 106 is equal to that of the PMOS transistor 107, the voltage across the resistive element 105 is equal to Vgsp1−Vgsp2. Expressions 1 and 2 together yield Expression 3 below.
Thus, the current I1 flowing through the resistive element 105 is expressed as shown in Expression 4 below.
Since the current flowing from the BGR-type current generation circuit 100 into the resistive load circuit 103 (the drain current of the PMOS transistor 110) is I1+I2 (=2·I1), the voltage Va at the node 114 is a voltage obtained by adding together the voltage across the resistive element 111 and the source-gate voltage of the PMOS transistor 110. Since the NMOS transistor 112 and the PMOS transistor 113 of the reference voltage output stage 104, the NMOS transistor 109 and the PMOS transistor 110 together form a current mirror-type source follower, the same voltage as the voltage Va is output from the reference voltage output stage 104 as the output voltage Vref. Thus, the output voltage Vref is expressed as shown in Expression 5 below.
V
ref
=Va=2R2I1+Vgsp3 Exp. 5
In Expression 5, Vgsp3 represents the source-gate voltage of the PMOS transistor 110.
Expressions 4 and 5 together yield Expression 6 below.
The gradient of Vref with respect to variations in the absolute temperature is expressed as shown in Expression 7 below, which is obtained by partially differentiating Expression 6 with respect to the absolute temperature T.
In Expression 7, the first term (R2·n·k·2·lnM)/(R1·q) takes a positive value, and the second term (∂Vgsp3/∂T) takes a negative value (e.g., about −1.5 mV/° C.). Thus, the voltage across the resistive element 111 has a positive coefficient with respect to the absolute temperature T, and the source-gate voltage Vgsp3 of the PMOS transistor 110 has a negative coefficient with respect to the absolute temperature T.
In the present embodiment, the resistance values R1 and R2 of the resistive elements 105 and 111 and the value M in the transistor size ratio 1:M between the PMOS transistors 106 and 107 are determined so that the temperature gradient of the output voltage Vref is zero. In other words, they are determined so that the value of Expression 7 is zero. The resistive elements 105 and 111 and the PMOS transistors 106 and 107 are designed so that R1, R2 and M are in the relationship as shown in Expression 8 below.
Thus, where the transistor size ratio between the PMOS transistors 106 and 107 is 1:M, the temperature coefficient of the output voltage Vref shown in Expression 7 can be made to be zero by designing the NMOS transistors 108 and 109 so that the transistor size ratio therebetween is 1:1 and by designing the resistive elements 105 and 111 so that R1 and R2 satisfy Expression 8. Since Expression 6 has no Vdd-dependent term, the output voltage Vref is not varied by variations in the potential Vdd of the drain-side power supply, provided that ideal elements are used.
The output impedance Z is expressed as shown in Expression 9 below.
In Expression 9, gm(N) denotes the transconductance of the NMOS transistor 112, and gm(P) the transconductance of the PMOS transistor 113.
Expression 9 indicates that the greater the static current I3 flowing through the reference voltage output stage 104, the more gm(N) and gm(P) increase and the output impedance Z decreases.
Thus, the output impedance can be decreased by providing the reference voltage output stage 104, instead of directly outputting the voltage Va at the node 114.
As compared with a case where the voltage Va at the node 114 is output directly, the provision of the reference voltage output stage 104 increases the overall current flow across the circuit by the static current flowing through the reference voltage output stage 104. In
In the reference voltage generation circuit of the present embodiment, two current paths merge together in the BGR-type current generation circuit 100 and extend as a single current path into the resistive load circuit 103. Therefore, the current consumption can be reduced more easily as compared with a case where the currents flowing through the two current paths are mirrored by the current mirror circuit and a current mirrored from the currents flows into a resistive load circuit formed along another current path. Moreover, the total circuit area is reduced because it is not necessary to provide elements for mirroring. Furthermore, the precision of the output voltage Vref is increased because there will be no situation where the current ratio between transistors used for mirroring is shifted from the desired current ratio due to variations among those transistors.
The reference voltage generation circuit of Embodiment 1 may be of a configuration as shown in
The BGR-type current generation circuit 116 includes a reference current generation circuit 117 and a current mirror circuit 118.
The reference current generation circuit 117 includes a resistive element 119, and NMOS transistors 120 and 121 (the reference current MOS transistors) whose transistor size ratio is M:1.
The current mirror circuit 118 includes PMOS transistors 122 and 123 (the current mirror MOS transistors) designed so that an equal source-drain current flows therethrough.
The value M and the resistance values R1 and R2 of the resistive elements 119 and 111 are determined so as to satisfy Expression 8. Thus, ideally, the output voltage Vref is not varied by variations in the power supply voltage.
Also with the configuration of
As shown in
The resistive load circuit 200 includes an NMOS transistor 201 (the load section MOS transistor) and a resistive element 202.
In the present embodiment, the NMOS transistor 201 and the NMOS transistor 112, together forming a current mirror circuit, are designed so that the source-drain current ratio therebetween is 1:N. The PMOS transistor 106 and the PMOS transistor 113, together forming a current mirror circuit, are designed so that the source-drain current ratio is 1:2N.
How the resistance values R1 and R2 of the resistive elements 105 and 202 and the value M are determined will now be described. The method for deriving the voltage produced by the resistive load circuit 200, i.e., the potential difference between the drain-side power supply and the node 114, is similar to Expressions 1 to 6, and will not be further described below. The output voltage Vref is obtained as shown in Expression 10 below.
In Expression 10, n is a constant dictated by the process, which typically is little dependent on the temperature and takes a value of about 1.4, for example. In the expression, k denotes the Boltzmann constant, T the absolute temperature, q the charge of electron, and Vgsp4 the gate-source voltage of the NMOS transistor 201.
The portion in the braces in Expression 10 is of the same pattern as the right-hand side of Expression 7, and therefore the values of M, R1 and R2 are determined so that the portion in the braces partially differentiated is zero. Thus, there is obtained the temperature-independent output voltage Vref, which is based on the potential Vdd. Ideally, the output voltage Vref is constant as long as the potential Vdd is constant.
Similar effects to those of Embodiment 1 are also realized in the present embodiment.
The reference voltage generation circuit of Embodiment 2 may be of a configuration as shown in
The value M, the resistance values R1 and R2 of the resistive elements 119 and 202 are determined so that the portion in the braces in Expression 10 partially differentiated is zero.
Also with the configuration of
As shown in
The reference current generation circuit 301 includes diodes 302 and 303 (the reference current diodes), a resistive element 304, and PMOS transistors 305 and 306 (the virtual short MOS transistors).
The diodes 302 and 303 are designed so that the diode size ratio therebetween is 1:M, whereby the reverse saturation current ratio therebetween is 1:M.
The PMOS transistors 305 and 306 are designed so that an equal source-drain current flows therethrough by, for example, using the same transistor size.
The resistance values R1 and R2 of the resistive elements 304 and 111 and the value M are determined so that there are little variations in the output voltage Vref with respect to variations in the temperature. How these values are determined in the present invention will now be described in detail.
Referring to
In Expression 11, Is denotes the reverse saturation current of the diode 302, k the Boltzmann constant, T the absolute temperature, and q the charge of electron.
Moreover, where the anode-cathode voltage of the diode 303 is denoted as Vd2, the current I12 flowing through the diode 303 is equal to the current I11, and therefore I11 can be expressed as shown in Expression 12 below.
Moreover, currents I11 and I12, which are equal to each other, flow through the PMOS transistors 305 and 306, respectively, whereby the source potentials of the PMOS transistors 305 and 306 are equal to each other.
Thus, the voltage across the resistive element 304 is Vd1−Vd2, which is expressed as shown in Expression 13 below, based on Expressions 11 and 12.
Based on Expression 13, the current I11 flowing through the resistive element 304 is expressed as shown in Expression 14 below.
Since the current flowing from the BGR-type current generation circuit 300 into the resistive load circuit 103, i.e., the current flowing through the resistive load circuit 103, is I11+I12(=2·I11), the voltage Va at the node 114 is a voltage obtained by adding together the voltage across the resistive element 111 and the source-gate voltage of the PMOS transistor 110. The NMOS transistor 112 and the PMOS transistor 113 of the reference voltage output stage 104 each form a current mirror-type source follower together with the NMOS transistor 109 and the PMOS transistor 110, respectively. Therefore, the reference voltage Vref is equal to the voltage Va. Thus, the output voltage Vref is expressed as shown in Expression 15 below.
V
ref
=V
a=2R2I11+Vgsp4 Exp. 15
In Expression 15, Vgsp4 denotes the source-gate voltage of the PMOS transistor 110.
Expressions 14 and 15 together yield Expression 16 below.
The gradient of Vref with respect to variations in the absolute temperature is expressed as shown in Expression 17, which is obtained by partially differentiating Expression 16 with respect to the absolute temperature T.
The first term (R2·k·2·lnM)/(R1·q) of Expression 17 takes a positive value, and the second term (∂Vgsp4/∂T) takes a negative value (e.g., about −1.5 mV/° C.). Thus, the voltage across the resistive element 111 has a positive coefficient with respect to the absolute temperature T, and the source-gate voltage Vgsp4 of the PMOS transistor 110 has a negative coefficient with respect to the absolute temperature T.
In the present embodiment, the constants R1, R2 and M are determined so that the temperature gradient of the output voltage Vref is zero. In other words, they are determined so that the value of Expression 17 is zero. Therefore, the resistive elements 304 and 111 and the diodes 302 and 303 are designed so that R1, R2 and M are in the relationship as shown in Expression 18 below.
Thus, where the diode size ratio between the diodes 302 and 303 is 1:M, the source-drain currents of the NMOS transistors 108 and 109 are equal to each other (i.e., the current ratio therebetween is 1:1) and the source-drain currents of the PMOS transistors 305 and 306 are equal to each other (i.e., the current ratio therebetween is 1:1), the temperature coefficient of the output voltage Vref shown in Expression 17 can be made to be zero by designing the resistive elements 304 and 111 so that R1 and R2 satisfy Expression 18. Since Expression 17 has no Vdd-dependent term, the output voltage Vref is not varied by variations in the potential Vdd of the drain-side power supply, provided that ideal elements are used.
Similar effects to those of Embodiment 1 are also realized in the present embodiment.
The reference voltage generation circuit of Embodiment 3 may be of a configuration as shown in
The reference current generation circuit 308 includes NMOS transistors 309 and 310 (the virtual short MOS transistors), diodes 311 and 312 (the reference current diodes), and a resistive element 313.
The NMOS transistors 309 and 310 are designed so that an equal source-drain current flows therethrough by, for example, using the same transistor size.
The diodes 311 and 312 are designed so that the diode size ratio therebetween is 1:M, whereby the reverse saturation current ratio therebetween is 1:M.
How the resistance values R1 and R2 of the resistive elements 313 and 202 and the value M are determined will now be described. The method for deriving the voltage produced by the resistive load circuit 200, i.e., the potential difference between the drain-side power supply and the node 114, is similar to Expressions 11 to 16, and will not be further described below. The output voltage Vref is obtained as shown in Expression 19 below.
In Expression 19, k denotes the Boltzmann constant, T the absolute temperature, q the charge of electron, and Vgsp4 the gate-source voltage of the NMOS transistor 201.
The portion in the braces in Expression 19 is of the same pattern as the right-hand side of Expression 16, and therefore the values of R1 and R2 are determined so that the portion in the braces partially differentiated is zero. Thus, there is obtained the temperature-independent output voltage Vref, which is based on Vdd. Ideally, the output voltage Vref is constant as long as Vdd is constant.
Similar effects to those of Embodiment 1 are also realized in the present embodiment.
Moreover, it is easier with diodes, than with MOS transistors, to realize little process variations. Therefore, as compared with a case where a BGR-type current generation circuit employed generates a current by utilizing the difference between the gate-source voltages of two MOS transistors as in Embodiments 1 and 2, it is easier to realize a more precise current in a case where a BGR-type current generation circuit employed generates a current by utilizing the difference between the anode-cathode voltages of two diodes as in the present embodiment.
As shown in
The reference current generation circuit 401 includes a pair of PMOS transistors 403 and 404 connected together in a cascode connection to the PMOS transistors 106 and 107, in addition to the configuration of the reference current generation circuit 101 of the reference voltage generation circuit shown in
As with the NMOS transistors 108 and 109, the NMOS transistors 405 and 406 are designed so that an equal source-drain current flows therethrough by, for example, using the same transistor size.
By arranging the MOS transistors of a BGR-type current generation circuit in a cascode current mirror configuration as described above, the resistance value between the first node and the second node becomes large, whereby there are little variations in the current I1 due to variations in the potential at the first node (the power supply potential). Thus, the constancy of the current I1 is much better than that with the BGR-type current generation circuit 100 of Embodiment 1.
The characteristics of the present embodiment can be incorporated into the reference voltage generation circuits of Embodiments 1 to 3 shown in
The reference voltage generation circuit of Embodiment 4 may be of a configuration as shown in
Also in a case where two pairs of MOS transistors together forming a current mirror structure as described above in Embodiment 4 are provided in the reference voltage generation circuits of Embodiments 1 to 3 shown in
With the reference voltage generation circuits of Embodiments 1 to 4 shown in
Specific circuit configurations applicable include a configuration as shown in
The reference voltage generation circuit shown in
The resistive load circuit 500 includes a resistive element 501 and a diode 502.
How the resistance values R1 and R2 of the resistive elements 313 and 501 and the value M are determined will now be described. The method for deriving the currents I1 and 12 flowing through the BGR-type current generation circuit 307 is similar to Expressions 11 to 14, and will not be further described below. Where the anode-cathode voltage of the diode 502 is denoted as Vd3, the output voltage Vref is obtained as shown in Expression 20 below.
V
ref=2R2I11Vd3 Exp. 20
Expressions 14 and 20 together yield Expression 21.
The gradient of Vref with respect to variations in the absolute temperature is expressed as shown in Expression 22, which is obtained by partially differentiating Expression 21 with respect to the absolute temperature T.
The first term (R2·k·2·lnM)/(R1·q) of Expression 22 takes a positive value, and the second term (∂Vd3/∂T) takes a negative value (e.g., about −2 mV/° C.). Thus, the voltage across the resistive element 501 has a positive coefficient with respect to the absolute temperature T, and the anode-cathode voltage Vd3 of the diode 502 has a negative coefficient with respect to the absolute temperature T.
The constants R1, R2 and M are determined so that the temperature gradient of the output voltage Vref is zero. In other words, they are determined so that the value of Expression 22 is zero. Therefore, the resistive elements 313 and 501 and the diodes 311 and 312 are designed so that R1, R2 and M are in the relationship as shown in Expression 23 below.
Thus, where the diode size ratio between the diodes 311 and 312 is 1:M, the source-drain currents of the PMOS transistors 122 and 123 are equal to each other (i.e., the current ratio therebetween is 1:1) and the source-drain currents of the NMOS transistors 309 and 310 are equal to each other (i.e., the current ratio therebetween is 1:1), the temperature coefficient of the output voltage Vref shown in Expression 22 can be made to be zero by designing the resistive elements so that R1 and R2 satisfy Expression 23. Since Expression 21 has no Vdd-dependent term, the output voltage Vref ideally is not varied by variations in the potential Vdd of the drain-side power supply.
In the reference voltage generation circuit of the present embodiment, two current paths extending from the drain-side power supply of the BGR-type current generation circuit 307 to the node 114 merge together and extend as a single current path into the resistive load circuit. Therefore, the current consumption can be reduced more easily as compared with a case where the currents flowing through the two current paths are mirrored by the current mirror circuit and a current mirrored from the currents flows into a resistive load circuit formed along another current path. For example, if a current of 0.5 μA is conducted through a first current path in the reference voltage generation circuit of
Moreover, the total circuit area is reduced because it is not necessary to provide elements for mirroring, as compared with a case where the currents flowing through the two current paths are mirrored by the current mirror circuit and a current mirrored from the currents flows into a resistive load circuit formed along another current path, as with the conventional configuration. Furthermore, the precision of the output voltage Vref is increased because there will be no situation where the current ratio between transistors used for mirroring is shifted from the desired current ratio due to variations among those transistors.
Moreover, diodes typically have less process variations than MOS transistors. Therefore, in a case where the diode 502 is used in the resistive load circuit 500 as in the present embodiment, as compared with a case where a MOS transistor is used, there are smaller variations in the output voltage Vref, and it is easier to realize a more precise reference voltage generation circuit.
Typically, the threshold voltage of a PMOS transistor can be made lower than the forward voltage of a diode. Therefore, in a case where a PMOS transistor is used in the resistive load circuit as in a configuration obtained by removing the reference voltage output stage 104 from the reference voltage generation circuit of
A reference voltage generation circuit shown in
The reference voltage generation circuit of
How the resistance values R1 and R2 of the resistive elements 304 and 501 and the value M are determined will now be described. The method for deriving the voltage produced by the resistive load circuit 500, i.e., the potential difference between the drain-side power supply and the node 114, is similar to Expressions 21 to 22, and will not be further described below. The output voltage Vref is obtained as shown in Expression 24 below.
In Expression 24, k denotes the Boltzmann constant, T the absolute temperature, q the charge of electron, and Vd3 the anode-cathode voltage of the diode 502.
The portion in the braces in Expression 24 is of the same pattern as the right-hand side of Expression 21, and therefore the values of R1 and R2 are determined so that the portion in the braces partially differentiated is zero. Thus, there is obtained the temperature-independent output voltage Vref, which is based on Vdd. Ideally, the output voltage Vref is constant as long as Vdd is constant.
Similar effects to those of Embodiment 5 are also realized in the present embodiment.
Referring to
Referring to
The reference voltage generation circuit of the present embodiment outputs the voltage at a node 602 as the output voltage Vref1 and the voltage at a node 601 as the output voltage Vref2.
How the resistance value R1 of the resistive element 105, the resistance value R2 of the resistive element 501 of the resistive load circuit 500 connected to the third node, the resistance value R3 of the resistive element 501 of the resistive load circuit 500 connected to the fourth node, and the value M in the transistor size ratio 1:M between the PMOS transistors 106 and 107 are determined will now be described. The anode-cathode voltage (forward voltage) of the diode 502 of the resistive load circuit 500 connected to the third node is denoted as VF1, and that of the diode 502 of the resistive load circuit 500 connected to the fourth node is denoted as VF2.
Below are expressions representing the temperature dependency of the output voltages Vref1 and Vref2. The method for deriving the current flowing through the two resistive load circuits 500 is similar to Expressions 1 to 5, etc., of Embodiment 1, and will not be further described below.
The output voltage Vref1 is expressed as shown in Expression 25 below.
The output voltage Vref2 is expressed as shown in Expression 26 below.
In Expressions 25 and 26, n is a constant dictated by the process, which typically is little dependent on the temperature and takes a value of about 1.4, for example. In the expression, k denotes the Boltzmann constant, T the absolute temperature and q the charge of electron.
The right-hand side of Expression 25 and the portion in the braces of the right-hand side of Expression 26 are of the same pattern as the right-hand side of Expression 6. By setting the ratio between R1 and R2 so that the right-hand side of Expression 25 is zero, there is obtained the temperature-independent output voltage Vref1, which is based on the source-side power supply potential Vss. By setting the ratio between R1 and R3 so that the portion in the braces of the right-hand side of Expression 26 is zero, there is obtained the temperature-independent output voltage Vref2, which is based on the drain-side power supply potential Vdd.
Thus, with the reference voltage generation circuit of the present embodiment shown in
In the reference voltage generation circuit of the present embodiment, two current paths merge together in the BGR-type current generation circuit 100 and extend as a single current path into the two resistive load circuits. Therefore, the current consumption can be reduced more easily as compared with a case where the currents flowing through the two current paths are mirrored by the current mirror circuit and a current mirrored from the currents flows into a resistive load circuit formed along another current path. Moreover, the total circuit area is reduced because it is not necessary to provide elements for mirroring. Thus, with the reference voltage generation circuit of the present embodiment, it is easy to generate a plurality of reference voltages with a small current consumption and a small circuit area.
In the present embodiment, the resistive load circuit 500 is used as each of the first and second resistive load circuits of
The reference voltage generation circuit of
The resistance value of the resistive element 701 can be adjusted by means of a laser trimming or anti-fusing process performed after circuit patterns are made in a wafer.
Where the anode-cathode voltage (forward voltage) of the diode 502 is denoted as VF1, Vref can be expressed as shown in Expression 27 below, i.e., with the same expression as that for Vref1 of Embodiment 6.
With the reference voltage generation circuit of the present embodiment, the resistance value of the resistive element 701 can be variably controlled. Therefore, if the forward voltage of the diode 502 is varied due to the process conditions, the output voltage Vref as shown in Expression 27 can be adjusted by controlling the resistance value of the resistive element 701.
Even with resistive load circuits other than the resistive load circuit 700, a resistive element whose resistance value can be adjusted can be used.
For example, a resistive load circuit 702 of the reference voltage generation circuit shown in
Vref is expressed by Expression 6 described above in Embodiment 1.
With the reference voltage generation circuit of
The reference voltage generation circuits of Embodiments 1 to 7 intrinsically have a bistability problem. A bistability problem is a problem that there is an abnormal stable state in addition to a normal stable state, and once the reference voltage generation circuit enters the abnormal stable state it will not return to the normal stable state. The normal stable state is a state where a current flows through the reference voltage generation circuit as described above in Embodiments 1 to 7 to normally generate the output voltage Vref. The abnormal stable state is a state where the gate voltage of the transistor of the BGR-type current generation circuit becomes stable at such a level that no current flows through the transistor. For example, the abnormal state is a state where the gate voltage of the PMOS transistors 106 and 107 of
A reference voltage generation circuit including a circuit for eliminating the bistability problem will now be described as a reference voltage generation circuit of Embodiment 8.
Referring to
The PMOS transistor 802 and the PMOS transistor 803 are turned ON by bringing a power-ON control signal XPON to the L level (the potential Vss). Thus, the PMOS transistor 802 and the PMOS transistor 803 can each serve as a switch.
The present embodiment is directed to a case where an initialization pulse that temporarily goes to the L level (the potential Vss) is input as the power-ON control signal XPON at the startup.
When the power-ON control signal XPON goes to the L level, the PMOS transistor 802 is turned ON, the source and the drain of the PMOS transistor 107 are shorted together, the gate voltage of the NMOS transistors 108 and 109 increases, and the gate voltage of the PMOS transistors 106 and 107 decreases. Therefore, even if the reference voltage generation circuit happens to be in an abnormal stable state where the gate voltage of the PMOS transistors 106 and 107 is the potential Vdd and the gate voltage of the NMOS transistors 108 and 109 is the potential Vss before the startup, the reference voltage generation circuit can be transitioned from the abnormal stable state to the normal stable state by bringing the power-ON control signal XPON to the L level at the startup.
The transition of the reference voltage generation circuit to the normal stable state can be made without the startup circuit 801 as long as the startup circuit 800 is provided. Without the startup circuit 801, however, the output voltage Vref output to the node 114 is substantially dependent on the potential Vdd.
In the present embodiment, where the startup circuit 801 is provided, the output voltage Vref at the startup is a voltage according to (controlled by) the gate-source voltage of the PMOS transistor 803 by turning ON the PMOS transistor 803 by bringing the power-ON control signal XPON to the L level. Therefore, by appropriately determining the transistor size of the PMOS transistor 803, it is possible to reduce the difference between the output voltage Vref at the startup and that during a normal operation. The circuit (b) in
The present embodiment may employ, as a switch, an NMOS transistor receiving at its gate a signal reversed from (complementary to) the power-ON control signal XPON, instead of the PMOS transistor 802.
The startup circuits 800 and 801 may be provided in the reference voltage generation circuit of Embodiment 1, in which case the circuit takes a configuration as shown in
The startup circuits 800 and 801 can be provided in the reference voltage generation circuits of Embodiments 2 to 7. The startup circuit 800 may be provided so that the transistor of the startup circuit 800 connects together the drain and the source of a first one of a pair of transistors provided in the reference current generation circuit and a pair of transistors provided in the current mirror circuit, wherein the drain of the first transistor is connected to the gate of a second one of the pairs of transistors, the second transistor being on the lower potential-side with respect to the first transistor. The startup circuit 801 can be provided so that the transistor of the startup circuit 801 controls the connection between the power supply to which the resistive load circuit is connected and the node 114, i.e., the connection between the second node and the third node (or the connection between the first node and the fourth node) in
The reference voltage generation circuit obtained by removing the reference voltage output stage 104 from the reference voltage generation circuits of
Alternatively, the resistive load circuit may employ either those elements in which a voltage thereacross is in proportion to the current therethrough with a positive proportionality constant, or those elements in which a voltage thereacross is in proportion to the absolute temperature with a negative proportionality constant. In such a case, however, the output voltage Vdd is dependent on the temperature. For example, if the resistive load circuit only includes a resistive element, the output voltage Vref will be lower, by the forward voltage of a diode, than that in a case where the resistive load circuit includes a resistive element and a diode, and the output voltage Vref will have a positive temperature coefficient.
In the reference voltage generation circuits of Embodiments 1 to 6 and 8 and variations thereof, the resistive element in the resistive load circuit may be replaced by a resistive element of Embodiment 7 whose resistance value can be adjusted.
The reference voltage generation circuit of the present invention is capable of generating a high-precision, stable voltage with a small current consumption and a small area, and is thus suitable as a band gap reference-type reference voltage generation circuit, or the like, for use in portable systems, battery-powered systems, integrated circuits provided therein, etc.
Number | Date | Country | Kind |
---|---|---|---|
2006-188348 | Jul 2006 | JP | national |