The invention relates to bandgap voltage references and particularly to bandgap voltage circuits operable in low supply voltage environments.
Bandgap voltage references and temperature dependent or temperature independent bias current generators are widely used in integrated circuits and have application in both bipolar and CMOS processes. Ultimately it will be understood that any bandgap based voltage or current generator provides for a combination of a Proportional To Absolute Temperature (PTAT) signal with a Complementary To Absolute Temperature (CTAT) signal. In bandgap voltage reference a base-emitter voltage of a bipolar transistor (which is CTAT) is added to a PTAT voltage generated from a base-emitter voltage difference of at least two bipolar transistors operating at different collector current density. In constant current generators or in current mode bandgap voltage generators two currents, one of the form of a PTAT current and one of the form of a CTAT current, are combined to generate a desired output current or voltage. In the design of such circuits operation at low power supply is desired.
An example of a known low voltage bandgap voltage reference implemented in CMOS process is presented in
Another example of a known prior art circuit configured to generate a constant current or with a predetermined temperature output voltage or current is presented in
There is therefore a need for a circuit that can operate in lower voltage supply environments but yet has a desired temperature behaviour.
Accordingly the invention provides a bandgap reference circuit which is operable in low supply conditions. Such a circuit includes a second amplifier and a resistor at the output of a bandgap reference cell to create a constant current summing node at which PTAT and CTAT currents are summed. In modifications to the circuit it is possible to also provide a voltage reference node corresponding to the signal provided at the summing node. A further modification enables generation of a second voltage reference whose value is related to the base emitter voltage Vbe of a bipolar transistor. Further modifications provided for the generation of curvature correction within the circuit by biasing each of the first and second bipolar transistors Q1 and Q2 with currents of different forms.
These and other features will be better understood with reference to the following drawings which will assist in an understanding of the teaching of the invention but which are not intended to be limiting in any fashion.
Exemplary implementations of circuits provided in accordance with the teaching of the invention are now described with reference to
A first example of such a circuit is presented in
The first transistor Q1 which is operable at the lower current density is coupled via the resistor R1 to the non-inverting input of the amplifier whereas the second transistor Q2, operable at the higher current density, is coupled directly to the inverting input of the amplifier. The voltage at the input to the amplifier is therefore related to the base emitter voltage Vbe of this second transistor Q1 and has a complementary to absolute temperature CTAT form.
A second amplifier A2 also having an inverting terminal, a non-inverting terminal and an output terminal is provided, the non-inverting terminal being coupled to the non-inverting terminal of the first amplifier A1. As a result the CTAT voltage Vbe at the input to the first amplifier A1 is reflected at the inputs of the second amplifier A2.
The inverting input of the second amplifier is coupled with the output of the first amplifier via the MOS devices MI and M2. The two MOS devices M1, M2 are desirably provided having the same aspect ratio W/L. Two degeneration resistors R3, R4 are also provided and are coupled between the sources of the two MOS devices M1, M2 and ground respectively. Each of the degeneration resistors R3, R4 are desirably provided having the same value. This will be understood as representing a preferred but not essential arrangement in that by scaling the MOS devices M1, M2 and their associated resistors R3, R4 to one another different scaled currents could be generated. The drains of the two MOS devices M1, M2 are coupled to each of the non-inverting and inverting inputs to the amplifier respectively.
The inverting input of the second amplifier A2 is also coupled via a first mirror arrangement provided by MOS devices M5, M4, M3 to the inputs to the first amplifier A1. The drain of the MOS device M5 is coupled to the inverting input of the second amplifier A2 and also to the drain of the second MOS device M2. It is also coupled to ground via a load resistor R2. It will be understood that assuming the MOS devices M1 and M2 have the same aspect ratio and the degeneration resistors R3 and R4 have the same value then the amplifier A1 forces the base-emitter voltage difference ΔVbe between Q1 and Q2 across resistor R1. As a result the drain currents of M1 and M2 are PTAT currents. All input voltages of A1 and A2 have substantially the same voltage level, which is base-emitter voltage Vbe of Q2 such that the voltage developed across R2 is the Vbe voltage which results in a CTAT current flowing through the load resistor R2. A summing node, I Sum, is therefore provided where this CTAT current which flows through R2 is summed with the PTAT current provided at the drain of M2. In this way the summed current at the summing node is derived from the CTAT and PTAT voltages.
A second mirroring arrangement is effected by coupling the gate of MOS device M5 to the gate of MOS device M6, which again is desirably provided having the same aspect ratio. As a consequence the drain current of M6 is substantially identical to the drain current of M5 which is equal to the current at the summing node. The drain current of M6 therefore is a constant current made up of a PTAT current and a CTAT current which flows through the load across which a constant voltage, V Sum, is developed. The voltage reference, and the originating current reference, can be scaled by scaling the relative values of the first and second resistors R1 and R2.
As M3, M4, M5 and M6 have the same gate-source voltage they will provide substantially identical drain currents. In this way although they are detailed as being first and second current mirrors, they provide the same mirroring of the current from the drain of M5 which is equal to the summed current. Depending on the resistor ratio of R2/R1, the drain currents of M3 to M6 can be provided as constant currents or with desired temperature behaviour. Assuming that the output is a constant current it will be understood that a constant current is provided at each of the drains of M3, M4, M5, M6 with the result that the first and second bipolar transistors Q1 and Q2 are biased with a constant current substantially equal to the summed current. It will be understood that the biasing of the first and second bipolar transistors Q1 and Q2 with a constant current provides for no compensation for second order temperature curvature effects but a modification to the circuit of
It will be understood that the value of the constant current/voltage nodes of
Referring now to
As was mentioned above, whereas in the circuit of
It will be appreciated that in the arrangement of
It will be understood that what has been described herein are exemplary arrangement of circuits that are operable in a bandgap configuration and can be used in environments with low supply voltages as there is no need to provide transistors in a cascoded arrangement. Such circuits may provide for simultaneous generation of temperature independent voltage and temperature independent current references. By providing a resistor at the output node of an amplifier it is possible to compensate for base emitter variations in the transistor providing the bandgap voltage cell CTAT component and this compensation can be achieved irrespective of the resistor's temperature coefficient. Such circuits may be configured to provide bias currents to each of the first and second bipolar transistors Q1 and Q2 as to compensate for second order curvature effects that are inherent in any bandgap cell.
It will be understood that what has been described herein are exemplary embodiments of circuits which, by providing a second amplifier and a resistor at the output of a bandgap reference cell it is possible to create a constant current summing node at which PTAT and CTAT currents are summed. In modifications to the circuit it is possible to also provide a voltage reference node corresponding to the signal provided at the summing node. A further modification enables generation of a second voltage reference whose value is related to the base emitter voltage Vbe of a bipolar transistor. Further modifications provided for the generation of curvature correction within the circuit by biasing each of the first and second bipolar transistors Q1 and Q2 with currents of different forms. While the present invention has been described with reference to exemplary arrangements and circuits it will be understood that it is not intended to limit the teaching of the present invention to such arrangements as modifications can be made without departing from the spirit and scope of the present invention. In this way it will be understood that the invention is to be limited only insofar as is deemed necessary in the light of the appended claims.
It will be understood that the use of the term “coupled” is intended to mean that the two devices are configured to be in electric communication with one another. This may be achieved by a direct link between the two devices or may be via one or more intermediary electrical devices.
Similarly the words comprises/comprising when used in the specification are used to specify the presence of stated features, integers, steps or components but do not preclude the presence or addition of one or more additional features, integers, steps, components or groups thereof.