The present invention is directed to integrated circuits and, more particularly, to a band gap reference voltage generator.
Reference voltage generators are used widely in integrated circuits (IC) and other electronic circuits to provide a reference voltage that is stable despite variations in fabrication processing conditions from one batch of products to another, and despite variations in operating temperatures. Various techniques are available for compensating the reference voltage for process variations, such as including trim resistors in the circuit design, which can be set or ‘trimmed’ when producing the IC.
Thermal compensation is commonly obtained by including a band gap module in the reference voltage generator. A band gap module includes forward-biased semiconductor PN junctions, which may be provided by diodes or by diode-connected bipolar junction transistors (BJT) or metal-oxide semiconductor field-effect transistors (MOSFET), for example. The voltage across a forward-biased semiconductor PN junction for a given current through the junction decreases with increasing temperature, commonly called complementary to absolute temperature (CTAT), varying by approximately −2 mV/° K in a silicon semiconductor, for example. A band gap module uses a voltage difference between a pair of matched forward-biased PN junctions operating at different current densities to generate a current that increases with increasing temperature, commonly called proportional to absolute temperature (PTAT). This current is used to generate a PTAT voltage in a resistor that is added to a CTAT voltage across a semiconductor PN junction, which may be one of the matched pair. The ratio of the PTAT and CTAT voltages may be set by setting resistance values, for example, so that the temperature dependencies of the PTAT and CTAT voltages compensate each other to a first order approximation. Typically, in a semiconductor device, the resulting voltage is about 1.2-1.3 V, close to the theoretical band gap of silicon at 0° K, 1.22 eV. The residual second order approximation of the temperature dependency typically is small within the operating temperature range around the temperature at which the ratio of the PTAT and CTAT voltages is set.
Trimming resistance values for the band gap module is conveniently performed digitally by setting switches or fuses to connect or short circuit trim resistors. It is desirable to be able to trim the resistance values bidirectionally about a central value, which is not the case in some known implementations. In some conventional implementations, it is necessary for the ON resistance of the trim switches to be small to reduce inaccuracy introduced by variability of their ON resistance, for example with variation of supply voltage. Trim switches with small ON resistance in conventional implementations tend to occupy a large area of the IC.
The present invention is illustrated by way of example and is not limited by embodiments thereof shown in the accompanying figures, in which like references indicate similar elements. Elements in the figures are illustrated for simplicity and clarity and have not necessarily been drawn to scale.
The trim resistor networks R7, R4/R5, and R6 carry currents that generate the voltage required across the resistance network. Examples of conventional resistance network are shown in
Referring now to
A second current conduction path 416 between the first node 404 and the second node 406 includes a second resistive element 418 connected in series between the first node 404 and a fourth node 420, and the second PN junction element Q2 which is connected in series between the fourth node 420 and the second node 406. A voltage error amplifier 422 has a first input connected to the tap 412, a second input connected to the fourth node 420, and an output 424 for providing a thermally compensated output voltage VREF. A feedback path 426 applies the output voltage VREF to a series connection of a third resistive element 428 with the first and second nodes 404 and 406.
In this example of the band gap reference voltage generator 400, the PN junction elements Q1 and Q2 comprise bipolar junction transistors (BJTs) having emitter, base and collector regions, the base regions being connected to the respective collector regions, and respective forward biased base-emitter junctions that are connected in series with the first and second current conduction paths 402 and 416. The plurality of first resistive elements 408 includes a plurality of resistive trim elements 430 and a plurality of connector elements 432 connecting the resistive trim elements 430 in series, the switch elements 414 being controllable to connect the tap 412 selectively with a connector element 432 and select a value of the voltage divider ratio at the tap 412, which is settable bidirectionally about a central value. This example of the band gap reference voltage generator 400 includes a controller for controlling the switch elements 414 to select and set the voltage divider ratio at the tap 412. The controller includes a trim register 434 and a decoder 436, which control a multiplexer including the switch elements 414. The first PN forward-biased junction element Q1 has a smaller current density than the second PN forward-biased junction element Q2 the ratio of the densities being M to 1, and the plurality of first resistive elements 408 presents a greater resistance than the second resistive element 418. The first input of the voltage error amplifier 422 is an inverting input and the second input of the voltage error amplifier is a non-inverting input.
In more detail, the plurality of first resistive elements 408 includes a resistor 438 having a resistance of R1-nR connected in series between the first node 404 and the resistive trim elements 430, a resistor 440 having a resistance of R2-nR connected in series between the second node 410 and the resistive trim elements 430, and the plurality of resistive trim elements 430 comprises a ladder of 2 n trim resistors of value R. The resistance presented in the first current conduction path 402 between the first node 404 and the third node 410 is independent of the voltage divider ratio and is equal to R1+R2. The resistance presented in the second current conduction path 416 by the second resistive element 418 is chosen to be equal to R1. The position of connection of the tap 412 to the ladder of 2 n trim resistors 430 of value R selected by the trim register 434 and the decoder 436 corresponds to a number k of the trim resistors 430, between −n and +n from the mid-point of the ladder of trim resistors 430 and selects the voltage divider ratio of the resistive elements 408, which is equal to R2/(R1+R2) when k is zero. The values of the resistances, including the resistor 428, and the bias voltages of the voltage error amplifier 422 are chosen so that nominally the output voltage VREF has a suitable value when the number k is equal to zero.
However, the actual characteristics of the voltage generator 400 are subject to variation due to manufacturing process variations, for example. The voltage divider ratio of the resistive elements 408 is adjusted by the trim register 434 and the decoder 436 during testing of the voltage generator 400 during production by measurement of the output voltage VREF compared to a standard reference voltage, at a specific temperature, to compensate for differences from the nominal characteristics of the voltage generator 400. The resistance R of the trim resistors 430 is chosen to be sufficiently small to provide a fine adjustment to the voltage divider ratio, while providing a sufficient range of fine adjustment without unduly increasing the number of trim resistors 430 and corresponding switch elements 414; in this example, it has been possible to limit the number of trim resistors 430 and corresponding switch elements 414 to sixteen. The value of the number k of the trim resistors 430 can be varied between −n and +n about the nominal value of zero, so that bidirectional adjustment is possible about the mid-point of the ladder of trim resistors 430 and, if the adjustment process overshoots, the direction of adjustment can be reversed, unlike with blowing fuses.
The voltage Vk at the tap 412 is applied to the inverting input of the amplifier 422 and the voltage drop VEB2 appearing at the node 420 is applied to the non-inverting input of the amplifier 422. For a given current and temperature, the voltage drop VEB1 across the BJT Q1, which has a current density M times less than the matched BJT Q2, is less than the voltage drop VEB2 across the BJT Q2. The plurality of first resistive elements 408 presents a greater resistance than the second resistive element 418, but the nominal values of the resistances R1, R2, R6 and R, are chosen so that the voltage Vk at the tap 412 is nominally equal to the voltage drop VEB2 across the BJT Q2 when the number k of the trim resistors 430 is equal to zero, corresponding to the mid-point of the ladder of 2 n trim resistors 430.
The negative feedback loop 426 makes the sum of the currents I1 and I2 in the resistor 428 and flowing respectively in the first and second current conduction paths 402 and 416 adjust to a level at which the voltage Vk and the voltage drop VEB2 at the inputs of the amplifier 422 are substantially equal.
The output voltage VREF can be represented as the sum of a constant biasing voltage and a thermally compensated correction fvbg. The voltage Vk at the tap 412 is given by:
V
k
=V
EB1
+I
1(R2+kR)
The voltage error amplifier 422 and the feedback loop 426 make the voltage Vk at the tap 412 substantially equal to the voltage drop VEB2 appearing at the node 420, so that:
V
k
=V
EB1
+I
1(R2+kR)=VEB2
The current I1 in the first current conduction path 402 is given by:
I
1
=ΔV
EB/(R2+kR),
where ΔVEB is the difference between the base-emitter voltage drops VEB2 and VEB1 across the BJTs Q2 and Q1, which is PTAT. The voltage between the nodes 404 and 406 is the same for the first and second current conduction paths 402 and 416, so that:
The Schockley diode equation gives:
V
EB1
≈V
T ln(I1/MIS), VEB2≈VT ln(I2/IS),
where IS is a normalized reverse-biased saturation current, much smaller than I1 or I2, VT is the thermal voltage given by k′T/q, where k′ is the Boltzmann constant, T is the absolute temperature in ° K and q is the charge of an electron, and where M is the ratio of current densities of the BJTs Q2 and Q1.
From the above, I1 is given by:
To a first order, if kR is much smaller than R1 and R2:
and:
From these equations, the value of the thermally compensated correction fvbg to the output voltage VREF can be derived as:
In these equations, M is a constant, C is a parameter that depends on M and on the ratios of two resistances, and the resistance ratio values can be made constant with temperature by matching their production process and design. The temperature coefficient of the output voltage VREF is measured with the number k equal to zero and thermal compensation can be achieved to a first order by adjusting the number k using the trim register 434, decoder 436 and the switch elements 414.
Only one of the switch elements 414 is turned ON at any one time, selecting the voltage divider ratio of the first resistive elements 408. The voltage error amplifier 422 presents a high input impedance. Accordingly, current flow through the ON switch element 414 is small and variation in its ON resistance has only a small effect on the performance of the band gap reference voltage generator 400 and a higher ON resistance can be tolerated readily. In the band gap reference voltage generator 400, the resistive trim elements 430 are all of equal value. In configurations as shown in
In the foregoing specification, the invention has been described with reference to specific examples of embodiments of the invention. It will, however, be evident that various modifications and changes may be made therein without departing from the broader spirit and scope of the invention as set forth in the appended claims. For example, the semiconductor substrate described herein can be any semiconductor material or combinations of materials, such as gallium arsenide, silicon germanium, silicon-on-insulator (SOI), silicon, monocrystalline silicon, the like, and combinations of the above. The PN junctions may be formed by diodes or diode-connected BJTs or MOSFETs or other transistors.
The connections as discussed herein may be any type of connection suitable to transfer signals from or to the respective nodes, units or devices, for example via intermediate devices. Accordingly, unless implied or stated otherwise, the connections may be direct connections or indirect connections. The connections may be illustrated or described in reference to being a single connection, a plurality of connections, unidirectional connections, or bidirectional connections. However, different embodiments may vary the implementation of the connections. For example, separate unidirectional connections may be used rather than bidirectional connections and vice versa. Also, a plurality of connections may be replaced with a single connection that transfers multiple signals serially or in a time multiplexed manner. Likewise, single connections carrying multiple signals may be separated out into various different connections carrying subsets of these signals. Therefore, many options exist for transferring signals.
Although specific conductivity types or polarity of potentials have been described in the examples, it will be appreciated that conductivity types and polarities of potentials may be reversed.
Also for example, in one embodiment, the illustrated examples may be implemented as circuitry located on a single integrated circuit or within a same device. Alternatively, the examples may be implemented as any number of separate integrated circuits or separate devices interconnected with each other in a suitable manner.
In the claims, the words ‘comprising’ and ‘having’ do not exclude the presence of other elements or steps then those listed in a claim. The terms “a” or “an,” as used herein, are defined as one or more than one. Also, the use of introductory phrases such as “at least one” and “one or more” in the claims should not be construed to imply that the introduction of another claim element by the indefinite articles “a” or “an” limits any particular claim containing such introduced claim element to inventions containing only one such element, even when the same claim includes the introductory phrases “one or more” or “at least one” and indefinite articles such as “a” or “an.” The same holds true for the use of definite articles. Unless stated otherwise, terms such as “first” and “second” are used to arbitrarily distinguish between the elements such terms describe. Thus, these terms are not necessarily intended to indicate temporal or other prioritization of such elements. The fact that certain measures are recited in mutually different claims does not indicate that a combination of these measures cannot be used to advantage.
Number | Date | Country | Kind |
---|---|---|---|
201210334326.9 | Sep 2012 | CN | national |