A bandgap reference voltage circuit provides an output reference that is insensitive to temperature, supply voltage and process variations. Bandgap reference voltage circuits are used in a wide variety of electronic circuits, such as wireless communication devices, memory devices, voltage regulators, filters, analog-to-digital converters, digital-to-analog converters and so on.
There are a variety of ways to generate a bandgap reference voltage that, in general, fall into two main categories. The first category is current mode generation of a bandgap reference voltage. The second category is voltage mode generation of a bandgap reference voltage.
In current mode generation of a bandgap reference voltage, current from a first current source that has a positive temperature coefficient is summed with current from a second current source that has a corresponding negative temperature coefficient to produce an output current. A bandgap reference voltage (VREF) is achieved by passing the output current through a resistance. The use of corresponding positive and negative temperature coefficients in the first and second current sources results in the effects of temperature being canceled out, thus stabilizing the bandgap reference voltage (VREF). For examples of bandgap reference voltage circuits that use current mode generation, see U.S. Pat. No. 5,666,046 and United States Patent Application number 2004/0155700A1.
In voltage mode generation of a bandgap reference voltage, a base-emitter voltage (VBE) is generated from a bipolar transistor having a negative coefficient. A thermal voltage (Vt) is generated that is proportional-to-absolute-temperature (PTAT). The thermal voltage (Vt) has a positive coefficient at room temperature. The thermal voltage is equal to the expression kT/q where k is Boltzmann's constant, T is absolute temperature, and q is the elementary electron charge constant. Neither k nor q is temperature-dependent, and the result is that thermal voltage (Vt) is directly proportional-to-absolute-temperature (PTAT). The thermal voltage (Vt) is multiplied by a constant (K) and summed with the voltage (VBE). The result is a reference voltage (VREF) that is described by Equation 1 below:
VREF=VBE+KVt EQUATION 1
For examples of voltage mode generation of a bandgap reference voltage, see for example, U.S. Pat. No. 4,849,684 and U.S. Pat. No. 5,900,773.
Current mode generation of a bandgap reference voltage has the ability to achieve a bandgap reference as low as approximately 1 volt. Additionally, current mode generation of a bandgap reference voltage can produce a programmable bandgap reference voltage as the output current has zero temperature coefficient. However, current mode generation of a bandgap reference voltage typically requires one or more relatively large resistors, which can result in a large chip size.
Voltage mode generation of a bandgap reference voltage requires smaller total resistance than current mode generation of a bandgap reference voltage, but typically cannot be used for generating a bandgap reference voltage less than about 1.2 volts. Also, using the voltage mode generation of a bandgap reference voltage, the resulting bandgap reference voltage typically is 1.2 volts or a positive integer multiple of 1.2 volts.
In accordance with an embodiment of the present invention, a reference voltage circuit includes first circuitry that generates a thermal voltage that is approximately proportional to absolute temperature, a first voltage multiplier, second circuitry that generates an inverse thermal voltage that is approximately inversely proportional to absolute temperature, a second voltage multiplier and a summer. The first voltage multiplier multiplies the thermal voltage to obtain a first multiplied voltage. The multiplied voltage is not equal to the thermal voltage. The second voltage multiplier multiplies the inverse thermal voltage to obtain a second multiplied voltage. The summer sums the first multiplied voltage with the second multiplied voltage to obtain a reference voltage.
A voltage generator 15 generates, at a location 20, a thermal voltage (Vt) that is proportional-to-absolute-temperature (PTAT). The thermal voltage (Vt) has a positive coefficient of, for example, +0.085 mV/° C. at room temperature. The thermal voltage is equal to the expression kT/q where k is Boltzmann's constant, T is absolute temperature, and q is the elementary electron charge constant. Neither k nor q is temperature-dependent, and the result is that thermal voltage (Vt) is directly proportional-to-absolute-temperature (PTAT). Thermal voltage (Vt) is multiplied by a voltage multiplier 16 that has a constant value K. Voltage multiplier 16 produces a signal with multiplied voltage (KVt) at a location 21. A voltage sum 17 sums the voltages of the signals at location 19 and location 21 and produces bandgap reference voltage (VREF) on output 22. Bandgap reference voltage (VREF) can be described as set out by Equation 2 below:
VREF=QVBE+KVt EQUATION 2
The constant value Q can be a fractional or an integer value. When Q is greater than 1, this results in bandgap reference voltage (VREF) being higher than the typical bandgap voltage of 1.2 volts (V). When Q is lower than 1, this results in bandgap reference voltage (VREF) being lower than the typical bandgap voltage of 1.2V. Selection of an appropriate value of Q allows any programmable reference voltage within the circuit range to be achieved. Minimum bandgap reference voltage (VREF) is, for example, about 1 volt.
Differentiating with respect to temperature and using the temperature coefficients for VBE and Vt leads to a set value of K and Q that should theoretically give zero temperature dependence. That is, bandgap reference voltage (VREF) has a zero first order temperature coefficient.
While herein, a base-emitter voltage (VBE) is used as an example of a voltage that is inverse to PTAT, the present invention works equally well when another type of voltage source that is inverse to PTAT is used instead of a base-emitter voltage (VBE). For example, a voltage source that is inverse to PTAT can be generated by a diode or another type of circuitry.
PTAT current source through circuit 300 includes a pnp bipolar transistor 301, a pnp bipolar transistor 302, an n-channel field effect transistor (FET) 321, an n-channel FET 322, a p-channel FET 331, a p-channel FET 332, a p-channel FET 333 and a resistor 311, connected as shown. VBE current source circuit 400 includes a pnp bipolar transistor 402, an n-channel FET 421, an n-channel FET 422, a p-channel FET 431, a p-channel FET 432, a p-channel FET 433 and a resistor 411, connected as shown. Sum circuit 500 includes a resistor 501, a resistor 502 and a node 510. Locations of a current IPT1, a current IPT2 a current IPT3, a current IBE1 a current IBE2, a current IBE3 are as shown. V311 is the voltage that occurs across resistance 311. The thermal voltage (Vt) is the fractional of the voltage V311. Base emitter voltage (VBE) is the voltage that occurs across resistance 411.
To achieve the PTAT current (IPT3), the thermal voltage Vt is generated across the resistor 311 using FETs 331, 332, 321 and 322 together with pn transistor diodes 301 and 302. FET 331, FET 332, FET 321 and FET 322 function as current mirrors. FET 331 and FET 332 are the same size. Likewise, FET 321, and FET 322 are the same size. This insures that current IPT1 is equal to current IPT2. The emitter area (A301) of PNP bipolar transistor 301 is scaled relative to the emitter area (A302), of PNP bipolar transistor 302. The scaling factor is designated by the variable “x” shown on
A301=x*A302 EQUATION 3
For example, bipolar transistor 301 and bipolar transistor 302 are fabricated in near proximity to each other and are well-matched so that bipolar transistor 301 and bipolar transistor 302 operate at the same emitter current. The difference (ΔVBE) in their base-to-emitter voltage is given by Equation 4 below:
ΔVBE=V311=(k*T/q)*In(x) EQUATION 4
The current IPT1 is also dependent on absolute temperature as demonstrated by Equation 5 below:
IPT1=IPT2=ΔVBE/R311=V311/R311=Vt*In(x)/R311 EQUATION 5
In Equation 4, V311 is the voltage dropped across resistor 311, the thermal voltage Vt is equal to (k*T/q) which is a fractional of V311 and R311 is the resistance of resistor 311.
Since FET 331, FET 332 and FET 333 form current mirrors, the current IPT3 is a multiple of IPT1. The size of FET 333 is M times the size of FET 331 (and M times the size of FET 332), which results in the current being magnified by a factor of M. Since IPT3/IPT1=M, this results in Equation 6 below:
IPT3=M*IPT1 EQUATION 6
Within VBE current source circuit 400, FET 431 and FET 432 are the same size. Likewise, FET 421 and FET 422 are the same size. Thus, current IBE1 and IBE2 are the same value. The values are given by Equation 7 below:
IBE1=IBE2=VBE402/R411 EQUATION 7
In Equation 7, R411 represents the resistance of resistor 411 and VBE402 represents the base-emitter voltage drop across transistor 402.
Since FET 431, FET 432 and FET 433 form current mirrors, the current IBE3 is a multiple of IBE1. FET 433 is N times the size of FET 431 and of FET 432, as represented by N shown on
IBE3=N*IBE1 EQUATION 8
Current IBE3 flows in to resistor 501 to generate part of the voltage drop across 501. The part of the voltage drop across 501 generated by IBE3 is represented by VBE
VREF
In Equation 9, Q=N*R501/R411 and R501 represents the resistance of resistor 501. By appropriately choosing the value of N, R501 and R411, the value of Q can be higher than one or lower than one.
The currents IPT3 and IBE3 are summed at node 510. The reference voltage VREF at node 201 can be generated as shown by Equations 10 below:
In Equations 10, R502 represents the resistance of resistor 502. With proper selection of values of K and Q the reference voltage VREF can be of any desired voltage within the range of the circuit. Further VREF is a first order temperature compensated reference voltage. Depending on the Q value, the VREF can be higher or lower than the typical bandgap voltage, 1.2V. If the value for Q is higher than 1, then VREF can be higher than 1.2V. If the value for Q is lower than 1, then the reference voltage is lower than 1.2V. The selection of K, that is, the selection of M and R502, depends on the value of Q, because K is used to compensate the negative temperature coefficient of the voltage VBE402.
For example, for a Chartered Semiconductor Manufacturing (CSM) 0.35 micrometer (μm) process where VCC=3 volts, x=8, M=N=1, R311=20 kilohm, R411=90 Kilohm, R501=36 kilohm and R502=37 kilohm it is possible to achieve VREF of approximately 0.5 volts that is almost independent of temperature. Likewise, for a CSM 0.35 μm process when VCC=3 volts, x=8, M=N=1, R311=20 kilohm, R411=40 Kilohm, R501=48 kilohm and R502=161 kilohm it is possible to achieve VREF of approximately 1.5 volts that is almost independent of temperature.
In another embodiment of the present invention, FET pair 321 and 322, and FET pair 421 and 422 can be replaced by operational amplifiers. An advantage of using operation amplifiers is that it can improve power supply voltage rejection ratio (PSRR) performance. An example circuit is shown in
PTAT current source through circuit 1300 includes a pnp bipolar transistor 1301, a pnp bipolar transistor 1302, an operational amplifier 1351, a p-channel FET 1331, a p-channel FET 1332, a p-channel FET 1333 and a resistor 1311, connected as shown. VBE current source circuit 1400 includes a pnp bipolar transistor 1402, an operational amplifier 1451, a p-channel FET 1431, a p-channel FET 1432, a p-channel FET 1433 and a resistor 1411, connected as shown. Sum circuit 1500 includes a resistor 1501, a resistor 1502 and a node 1510. Locations of a current IPT1, a current IPT2, a current IPT3, a current IBE1, a current IBE2, a current IBE3, x, M and N are as shown. V1311 is the voltage that occurs across resistance 1311, the thermal voltage Vt is equal to (k*T/q) which is a fractional of V1311. Base emitter voltage (VBE1402) is the voltage that occurs across resistance 1411.
In another embodiment of the present invention, pnp bipolar transistor 1402 can be eliminated and the base emitter voltage across pnp bipolar transistor 1302 can be used in place of the base emitter voltage across pnp bipolar transistor 1302. This is illustrated by
PTAT current source through circuit 2300 includes a pnp bipolar transistor 2301, a pnp bipolar transistor 2302, an operational amplifier 2351, a p-channel FET 2331, a p-channel FET 2332, a p-channel FET 2333 and a resistor 2311, connected as shown. VBE current source circuit 2400 includes an operational amplifier 2451, a p-channel FET 2431, a p-channel FET 2433 and a resistor 2411, connected as shown. Sum circuit 2500 includes a resistor 2501, a resistor 2502 and a node 2510. Locations of current IPT1, a current IPT2, a current IPT3, a current IBE1, a current IBE3, x, M and N are as shown. V2311 is the voltage that occurs across resistance 2311, the thermal voltage Vt is equal to (k*T/q) which is a fractional of V2311. Base emitter voltage (VBE2302) is the voltage that occurs across resistance 2411.
In another embodiment of the present invention multiple reference voltages can be generated. Each reference voltage can have a different voltage level and all can be independent of temperature. This is illustrated by
PTAT current source through circuit 3300 includes a pnp bipolar transistor 3301, a pnp bipolar transistor 3302, an n-channel FET 3321, an n-channel FET 3322, a p-channel FET 3331, a p-channel FET 3332, a p-channel FET 3333, a p-channel FET 3334, a p-channel FET 3335 and a resistor 3311, connected as shown. VBE current source circuit 3400 includes a pnp bipolar transistor 3402, an n-channel FET 3421, an n-channel FET 3422, a p-channel FET 3431, a p-channel FET 3432, a p-channel FET 3433, a p-channel FET 3434, a p-channel FET 3435 and a resistor 3411, connected as shown. Sum circuit 3500 includes a resistor 3501, a resistor 3502, a resistor 3503, a resistor 3504, a resistor 3505, a resistor 3506, a node 3510, a node 3511 and a node 3512. Locations of a current IPT1, a current IPT2, a current IPT3, a current IPT4, a current IPT5, a current IBE1, a current IBE2, a current IBE3, a current IBE4 a current IBE5 x, M, M1, M2, N, N1 and N2, are as shown. V3311 is the voltage that occurs across resistance 3311, the thermal voltage Vt is equal to (k*T/q) which is a fractional of V3311. Base emitter voltage (VBE3402) is the voltage that occurs across resistance 3411.
By appropriately selecting values of M, M1, M2, N, N1, N2, and the values of resistors 3501, 3502, 3503, 3504, 3505 and 3506, resulting in different values for K and Q, different voltage references for VREF, VREF1, VREF2 can be generated. In alternative embodiments (not shown), operational amplifiers can be used to replace the n-channel FETs shown in
In the circuits shown in
PTAT current source through circuit 4300 includes a pnp bipolar transistor 4301, a pnp bipolar transistor 4302, an operational amplifier 4351, a p-channel FET 4331, a p-channel FET 4332, a p-channel FET 4333 and a resistor 4311, connected as shown. VBE current source circuit 4400 includes an operational amplifier 4451, an operational amplifier 4452, a resistor 4412, a resistor 4413, a resistor 4414 and a resistor 4415, connected as shown. Sum circuit 4500 includes a resistor 4502 and a node 4510. Locations of current IPT1, a current IPT2 and a current IPT3, a current IBE1, a current IBE3, x and M are as shown. V4311 is the voltage that occurs across resistance 4311, the thermal voltage Vt is equal to (k*T/q) which is a fractional of V4311. Base emitter voltage (VBE) is the voltage (VBE4302) that occurs across pnp bipolar transistor 4302. As shown in
For
The foregoing discussion discloses and describes merely exemplary methods and embodiments of the present invention. As will be understood by those familiar with the art, the invention may be embodied in other specific forms without departing from the spirit or essential characteristics thereof. Accordingly, the disclosure of the present invention is intended to be illustrative, but not limiting, of the scope of the invention, which is set forth in the following claims.
Number | Name | Date | Kind |
---|---|---|---|
4849684 | Sonntag et al. | Jul 1989 | A |
5614816 | Nahas | Mar 1997 | A |
5666046 | Mietus | Sep 1997 | A |
5900773 | Susak | May 1999 | A |
6366071 | Yu | Apr 2002 | B1 |
6563371 | Buckley, III et al. | May 2003 | B2 |
7199646 | Zupcau et al. | Apr 2007 | B1 |
20040155700 | Gower et al. | Aug 2004 | A1 |
20050231270 | Washburn | Oct 2005 | A1 |
20060061412 | Molina et al. | Mar 2006 | A1 |
Number | Date | Country | |
---|---|---|---|
20070080741 A1 | Apr 2007 | US |