The present disclosure relates to microelectronic circuits and more specifically to a bandgap reference circuit for generating a substantially temperature independent voltage or current.
A bandgap reference circuit is a functional block of an integrated circuit or system that can generate a voltage or current that does not change significantly with temperature. In other words, a bandgap reference can have a temperature coefficient (TC) that is relatively flat over a range of temperatures (e.g., 0-60 degrees C.). The relatively flat temperature coefficient may be generated by summing a current source that is proportional to absolute temperature with a current source that is complementary to absolute temperature. The temperature dependence of the proportional and complementary current sources, when combined, cancel each other to produce a reference current that is relatively insensitive to temperature. The current source that is proportional to absolute temperature and the current source that is complementary to absolute temperature may also be used to generate a reference voltage that is relatively insensitive to temperature.
However, especially with low power applications, known bandgap reference circuits still suffer from deleterious output noise and temperature variability. Low-power, current-mode bandgap references can require large value resistor(s) to generate an output voltage with a desired value, for example in near 1.2V. The output noise of a current-mode bandgap reference circuit is proportional to the resistance value. To decrease the output voltage noise of a current-mode bandgap, one may decrease the value of the resistance and thus increase the current value to maintain the output voltage. However, such solutions result in more power consumption. Another approach to decrease the output voltage noise of a current-mode bandgap may be to add a low-pass filter at the output. Nevertheless, the required capacitor value may be too high (i.e., in the range of 100s of nano-farads (nF)) which makes its integration on-chip unpractical in some cases. Moreover, to reduce low-frequency noise (i.e., flicker noise) in the current-mode bandgap, large area transistors may be used which in turn significantly increases the silicon area of the bandgap. Techniques are needed to improve the temperature variability of bandgap reference circuits, as well as their output noise. Further, techniques are needed to reduce the on-die area of bandgap reference circuits.
The present disclosure may be better understood, and its numerous features and advantages made apparent to those skilled in the art by referencing the accompanying drawings, in which:
The use of the same reference symbols in different drawings indicates similar or identical items. Unless otherwise noted, the word “coupled” and its associated verb forms include both direct connection and indirect electrical connection by means known in the art, and unless otherwise noted any description of direct connection implies alternate embodiments using suitable forms of indirect electrical connection as well.
CTAT current generator 102 generates a CTAT current, in this example based on a base-emitter voltage (VBE) of a transistor divided by a resistance R, and incudes source degeneration using a source a source degeneration resistor, as further discussed below. The generated CTAT current is mirrored in first CTAT current mirror 106, which includes temperature co-adjustment and source degeneration. The generated CTAT current is also mirrored in second CTAT current mirror 110, which includes source degeneration.
PTAT current generator 104 generates a PTAT current, and includes chopper circuits 105 to reduce output voltage noise and improve current matching and temperature stability, as further discussed below. First PTAT current mirror 108 also includes temperature co-adjustment and source degeneration. First PTAT current mirror 108 mirrors the PTAT current and feeds it to current summing node 107. Second PTAT current mirror 112 also mirrors the PTAT current, and includes source degeneration. Second PTAT current mirror 112 feeds its mirrored current to current summing node 113.
Current summing node 107 is connected to an output 109 for providing a reference current IOUT. Current summing node 113 is connected to an output resistor for creating a reference voltage VOUT at output terminal 114.
Bandgap reference circuit 200 includes a PTAT current generator 210, a CTAT current generator 220, a first CTAT current mirror 230, a first PTAT current generator 240, a second CTAT current mirror 250, a second PTAT current generator 260, a reference voltage output 270 providing a referenced voltage labeled “VREF”, and a reference current output 280 providing a reference current labeled “IREF”.
PTAT current generator 210 includes two branches 215 and 216 functioning as a current mirror with source degeneration. PTAT current generator 210 includes source degeneration resistors RSD1 and RSD2, a PTAT current generator input PMOS transistor MP1, a PTAT current generator output PMOS transistor MP2, a chopper circuit 211, cascode PMOS transistors MP3 and MP4, an NMOS transistor MNR1, a PMOS transistor MPR1, two NMOS cascode transistor MN1 and MN2, a chopper circuit 212, two NMOS bias transistors MN1 and MN2, a chopper circuit 213, a resistor R1, and two bipolar junction transistors (BJTs) Q1 and Q2.
Generally, PTAT current generator 210 generates a PTAT current “IPTAT” through transistor Q2 and mirrors that current in transistor Q1. Referring to the two branches 215 and 216, source degeneration resistor RSD1 is connected between an upper rail voltage and a source terminal of a PMOS transistor MP1, and source degeneration resistor (RSD2) is connected between the upper rail voltage and a source terminal of a PMOS transistor MP2. PMOS transistors MP1 and MP2 have their gates connected to each other. Chopper circuit 211 alternately connects the drain terminal of the PMOS transistor MP1 to the source terminals of MP3 and MP4 and connects the drain terminal of MP2 to the source terminals of MP4 and MP3. The drain of cascode PMOS transistor MP3 is connected to the gates of PMOS transistors MP1 and MP2.
NMOS transistor MNR1 has a drain connected to the drain of PMOS transistor MP3, and PMOS transistor MPR1 has a source connected to the drain of PMOS transistor MP4. NMOS transistor MNR1 and PMOS transistor MPR1 act as resistors (MOS in triode region), and may be replaced by resistors in some embodiments. NMOS transistor MNR1 and PMOS transistor MPR1 are employed in this embodiment and operated in a triode region in order to save die area. The gate of PMOS transistor MPR1 driven by a tied-low voltage “VTL” to achieve the proper bias, and the gate of NMOS transistor MNR1 is driven by a tied-high voltage VTH” for the same reason.
The drain of cascode NMOS transistor MN3 is connected to the gate of NMOS transistors MN1 and MN2, and the drain of cascode NMOS transistor MN4 is connected to the source of NMOS transistor MNR1. The gates of cascode NMOS transistors MN3 and MN4 are connected to the drain of transistor MP4. The source of cascode NMOS transistor MN3 is alternately connected to the drain of MN1 and to the drain of MN2 whereas MN4 is alternately connected to MN2 and MN1 using the chopper circuit 212. NMOS transistor MN1 and MN2 have their gates connected to the drain of PMOS transistor MPR1. The source of NMOS transistors MN1 is alternately connected to the emitter of transistor Q1 and to the resistor R whereas the source of MN2 is alternately connected the resistor R1 and the emitter of the transistor Q1 using the chopper circuit 213. The other terminal of resistor R1 is connected to the emitter of transistor Q2. Transistors Q1 and Q2 have their collector terminals and base terminals connected to the circuits ground or negative voltage rail in a diode arrangement. Transistors Q1 and Q2 maybe replaced by NPN transistors in some embodiments.
Each of chopper circuits 211, 212, and 213 includes four switches which are driven with a clock signal “CLK” as depicted in the expanded view of chopper circuit 213 depicted on the right. Each chopper circuit 211, 212, and 213 in this embodiment includes four terminals labeled “M”, “N”, “P”, and “Q”. The clock signal CLK is fed to a non-overlap clock circuit 214 which produces two clock signals “f1” and “f2”, which each drive two of the four switches in a non-overlapping fashion such that the switches driven by clock signal f1 are closed when the switches driven by clock signal f2 are open, and vice versa.
In operation, PTAT current generator 210 generates matching currents to bias transistors MN1 and MN2. Accordingly, a gate-source voltage (VGS) of NMOS transistor MN1 can substantially match (e.g., equal) a gate-source voltage of NMOS transistor MN2. Current from MN1 generates a first base-emitter voltage VBE1 across transistor Q1 and the (matching) current from MN2 generates a second base-emitter voltage, VBE2, across transistor Q2. Transistors Q1 and Q2 may be sized differently. For example, Q2 may be 8 times the size of Q1. In this situation, the base-emitter voltage across each transistor may be different, and the PTAT current (IPTAT) may be given as the difference in the base-emitter voltages (ΔVBE) divided by the resistance of R1.
Source degeneration resistors RSD1 and RSD2 improve (i.e., make more accurate) the mirroring of the PTAT current by reducing a random mismatch of the pairs of transistors. The PTAT current generator is in a cascode configuration to improve the mirroring of the PTAT current by reducing systematic mismatches. Additionally, the cascode configuration can boost an output impedance of the PTAT current generator 210. Random mismatches may include variations in device parameters (e.g., device length, channel doping, oxide thickness, etc.) due to random variations in the lithography and/or other processes used for fabricating the devices. Systematic mismatches, however, may still exist. Systematic mismatches may include variations in circuit operation due to the design (e.g., topology) and/or the layout of the circuit.
CTAT current generator 220 includes a source degeneration resistor RSD3, two PMOS transistors MP5 and MP8, an NMOS transistor MNR2, an amplifier 221, an PMOS transistor 222 and a resistor R2, all connected in series between the upper rail voltage and the lower rail voltage. The base-emitter voltage (VBE1) of transistor Q1 is coupled to resistor R2 using amplifier 221, with an output connected to the gate of PMOS transistor 222. The first base-emitter voltage across resistor R2 generates a CTAT current “ICTAT”. While in this implementation, the transistor 222 is a p-type transistor, other transistor types may be used. For this implementation, the inverting input of the amplifier 221 is coupled to transistor Q1. The present disclosure is not limited to this configuration. For example, transistor 222 may be an n-type transistor, or the non-inverting input of the amplifier is coupled to transistor Q1.
PMOS transistor MP5 is connected in a cascode configuration with PMOS transistor MP8, with the gate of PMOS transistor MP5 connected to the drain of PMOS transistor MP8 at a node labeled “vgc”. NMOS transistor MNR2 is connected between the drain of PMOS transistor MP8 and the source of transistor 222, and has its gate connected to the voltage VTH (tie high voltage) to bias it to act as a resistor. As discussed with respect to transistors MPR1 and MNR1, a resistor may be used in place of NMOS transistor MNR2. The source of NMOS transistor MNR2 is connected to the gate of PMOS transistor MP8 at a node labeled “vgc_cas”.
CTAT current mirror 230 is connected to CTAT current generator 220 to mirror the CTAT current ICTAT. CTAT current mirror 230 includes a source degeneration resistor RSD4, two PMOS transistors MP6 and MP9, and a resistor R3, all connected in series between the upper rail voltage and the lower rail voltage. The gate of PMOS transistor MP6 is connected to the gate of PMOS transistor MP5, and the gate of PMOS transistor MP9 is connected to the gate of PMOS transistor MP8, providing a current mirror of the cascode circuit of CTAT current generator 220.
Similarly, PTAT current mirror 240 is connected to PTAT current generator 210 to mirror the PTAT current IPTAT. PTAT current mirror 240 includes a source degeneration resistor RSD5, and two PMOS transistors MP7 and MP10, and a resistor R3, all connected in series.
In this embodiment, CTAT current mirror 230 and PTAT current mirror 240 both feed their current through resistor R3 to create a reference voltage labeled “VREF” proportional to the sum of their mirrored currents. Reference voltage VREF is provided at a node 270. A resistor RF is connected between a positive node of resistor R3 and node 270, and a capacitor CF is connected between node 270 and the lower voltage rail, providing low-pass filtering of reference voltage VREF.
A second set of current mirrors, CTAT current mirror 250 and PTAT current mirror 260, are present in this embodiment to provide a reference current “IREF” at node 280. While both a reference current and a reference voltage are made available as outputs in this embodiment, either one may be provided alone in other embodiments. CTAT current mirror 250 is connected to CTAT current generator 220 to mirror the CTAT current ICTAT. CTAT current mirror 250 includes two lowpass filters (LPF's) 227 and 228, a source degeneration resistor RSD6, two PMOS transistors MP11 and MP12, connected in series between the upper rail voltage and an output terminal 280. The gate of PMOS transistor MP11 is coupled to the gate of PMOS transistor MP5 through LPF 227. The gate of PMOS transistor MP12 is coupled to the gate of PMOS transistor MP8 through LPF filter 228.
PTAT current mirror 260 is connected to PTAT current generator 210 to mirror the PTAT current IPTAT. PTAT current mirror 240 includes a source degeneration resistor RSD7, and two PMOS transistors MP13 and MP14 connected in series between the positive voltage rail and output terminal 280. The gate of PMOS transistor MP13 is coupled to the gate of PMOS transistor MP1 through a LPF 217. The gate of PMOS transistor MP14 is coupled to the gate of PMOS transistor MP3 through a LPF filter 218.
The mirrored PTAT and CTAT currents from CTAT current mirror 250 and PTAT current mirror 260 are combined as shown as reference current IREF which is fed to output terminal 280.
In operation, bandgap reference circuit 200 includes a CTAT current mirror using source degeneration resistors RSD5 and RSD4 to improve (i.e., make more accurate) the mirroring of the CTAT current by reducing a random mismatch of the opposing transistors in branches 215 and 216. The CTAT current mirror is in a cascode configuration (i.e., a cascode CTAT current mirror 220) to improve the mirroring of the CTAT current by reducing a systematic mismatch. Additionally, the cascode configuration can boost an output impedance of the CTAT current mirror.
Bandgap reference circuit 200 includes a set of variable resistors (e.g., R2, R3, RSD4, RSD5, RSD6, and RSD7) that can be adjusted (e.g., trimmed) to change a value of the reference voltage or reference current at a particular temperature, or a rate of change of the reference voltage or reference current over a range of temperatures.
A reduction of the output voltage noise of the current-mode bandgap is achieved in some embodiments using source degeneration on the current mirrors and chopping on the transistor devices contribute the most to the output voltage noise.
The source degeneration on the current also improves the matching performance and, especially in combination with the chopper circuits, and provides one or more of several advantages, as further discussed below. First, there is a reduction of the TC variability due to mismatch. Second, there is a reduction of ripples on the output voltage due to mismatch and the use of chopper circuits. Third, there is a reduction of the need to filter the output using large value capacitor. As a result, only a small filtering capacitor (CF) may be needed to filter the chopper glitches. Fourth, the bandgap reference circuit is made more suitable for low-power applications. Fifth, the noise is be reduced even when the output current is relatively low (on the order of nano-amperes (nA)). Sixth, the bandgap reference circuit does not require large area transistors to reduce the flicker noise. Seventh, the bandgap reference circuit generates a current-reference with very low TC.
The matching performance of a current mirror can be highly dependent on its region of operation. For a current mirror without source degeneration (i.e., for a current mirror in which the input resistor Ri and the output resistor Ro are zero), the relative source-drain current error for a MOS transistor in the current mirror is given by the equations below.
is related to the operating region of transistor (i.e., weak inversion, moderate inversion and strong inversion).
In the above equation, W and L are respectively the gate-width and the gate-length of the transistor, AvTH and Aβ the proportionality constants which are technology-dependent, β=μCOXW/L, μ the carrier mobility, and COX the gate-oxide capacitance per unit area.
The transconductance-to-current ratio (gm/l) is the only parameter in equation (1) that is bias dependent while σ(ΔVTH) and
depend on the technology and the transistor area (e.g., WL). The transconductance-to-current ratio is strongly related to the transistor operation. The transconductance-to-current ratio is high (e.g., maximum) value when the MOS transistor is in a weak inversion region, is lower when the MOS transistor is operated in a moderate inversion region and is still lower when the MOS transistor is operated in a strong inversion region.
For the current mirror without source degeneration (i.e., Ro=Ri=0) operating in the weak inversion region, the transconductance-to current ratio of the transistor can be expressed by the equations below.
To decrease the source-drain current error, the area (e.g., WL) of the transistor can be increased and the transconductance-to-current ratio can be reduced. The transconductance-to-current ratio can be reduced by decreasing the W/L ratio of the transistor to move the operating point from weak inversion towards strong inversion while keeping a large transistor area. Simply increasing the size of a transistor, however, can require more physical (die) area. Instead of these approaches, the disclosed current mirror is configured to decrease the transconductance-to-current ratio (and thus the relative source-drain current error) using source degeneration (i.e., Ro>0, Ri>0). When these input and output resistors are non-zero, the effective transconductance, Gm, can be expressed by the equation below.
Where Rs is Ro and/or Ri, if Rs>>1/gm, then Gm is approximately 1/Rs. Using this approximation, the transconductance-to-current ratio can be given by the equation below,
Source degeneration as used herein also reduces the output current noise in terms of noise and considering only the flicker noise. For simple current mirror, the output current noise PSD is:
I
out
2
For a current mirror with source degeneration the output current noise PSD is:
For the current-mode bandgap circuit of
V
ref=(IPTAT+ICTAT)R (10)
For the sake of simplicity,
The output voltage noise can be expressed as:
Where
(
For low-power applications, in which the current is on the order of nano-amperes (nA), the resistor R has a value of tens of megaohms (MΩ) which leads to a high output voltage noise.
By adding a source degeneration on the current mirrors as shown in
This addition further reduces the CTAT and PTAT core contribution in
Thus, various embodiments of a bandgap reference circuit, an IC including such a circuit, and a corresponding method have been described. The various embodiments provide a bandgap reference capability suitable for low-power applications (with current in nA) requiring high-accuracy and low noise. The techniques herein provide noise reduction of at least 3.5-fold compared to an implementation without choppers and source degeneration. They also provide improvement of the temperature stability (the PPM/C STD is 3 times smaller compared to an implementation without choppers and source degeneration). They also provide reduction of the output ripples by improving the matching performances due to the source degeneration. Furthermore, the circuits herein utilize a relatively small silicon area in achieving such results.
The above-disclosed subject matter is to be considered illustrative, and not restrictive, and the appended claims are intended to cover all such modifications, enhancements, and other embodiments that fall within the true scope of the claims.
Thus, to the maximum extent allowed by law, the scope of the present invention is to be determined by the broadest permissible interpretation of the following claims and their equivalents, and shall not be restricted by the forgoing detailed description.
This application claims the benefit of U.S. Provisional Patent Application No. 63/269,051 filed on Mar. 9, 2022 which is incorporated by reference in its entirety. This application also claims the benefit of U.S. Provisional Patent Application No. 63/373,244 filed on Aug. 23, 2022 which is incorporated by reference in its entirety.
Number | Date | Country | |
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63269051 | Mar 2022 | US | |
63373244 | Aug 2022 | US |