The present invention relates generally to voltage references in transistor circuitry, and particularly to the use of switch capacitors in BGREF circuitry.
With advances in Internet of Thing (IoT) applications and the expansion of mobile devices, energy consumption has become a primary focus of attention in integrated circuits design. These mobile battery operated devices need to operate for extended periods without recharging and therefore requiring ultra-low energy consumption. Many IoT devices require operation in a wide range of frequencies that are dynamically defined by the application. Low voltage operation in the “near-threshold” region has been shown to be the ideal way to dramatically reduce energy dissipation, still achieving reasonable performance. However, an aggressive scaling of supply voltage results in performance degradation and a much higher sensitivity to process variations and temperature fluctuations.
In addition to the reduction in supply voltage, many of the circuits are duty cycled, and turned off during sleep states. However, there are several types of circuits which need to be “always-on” and operate during standby mode. Among these circuits are real-time-clocks (RTC) and power management circuits, such as low drop out regulators (LDO) and DC-to-DC converters. All of these always-on elements require analog voltage and current references. To meet these requirements, there has been significant recent interest in ultra-low power references.
One such reference known in the prior art is the so-called 2T (two terminal) transistor-based voltage reference, which uses two MOSFET transistors sized such that the temperature coefficients of their threshold voltages (Vth) cancel out, thereby yielding a voltage reference which is temperature independent. Another 2T version uses native zero threshold devices which can produce a reference voltage independent of Vdd with only two transistors. Although the 2T references are very attractive due to their simplicity and ultra-low power (pW range), they have not yet found acceptance in most IOT systems. This is because the temperature coefficient of Vth is not necessarily guaranteed by the process, especially in advanced nodes. In general the use of the temperature dependence of Vth in MOS devices is not considered reliable in real products, since it can change over the course of the product lifetime, due to speed up of the process.
Many computer systems utilize reference voltages produced by the parasitic Bipolar Junction Transistor (BJT), a.k.a. diode based references. The most common of these is shown in
where Ic is the collector current, Vbe is the base-emitter voltage, Vg00 is the extrapolated Vbe at 0K, K=Boltzmann constant, q=electron charge, λ is its linear temperature coefficient and T is the absolute temperature. Using equation 1, the CTAT (complimentary to absolute temperature) and PTAT (proportional to absolute temperature) terms can be calculated for the circuit in
The utility of this circuit is that both the voltage and temperature coefficient of Vref can be trimmed by digitally adjusting R3 and R2* respectively. Note that the terms PN diode and BJT are used interchangeably throughout the specification and claims. Essentially, the PN Junction Diode is the parasitic PNP BJT in the CMOS process whose base and collector are both connected to Vss (or ground).
One of the limitations and disadvantages of prior art nW BGREF's is very large area, since the low currents necessitate the use of very large resistors in order to generate a significant voltage across them. Another disadvantage is that due to the low currents, the wakeup times of these references can be in the milli-second range.
The present invention seeks to provide a novel use of switch capacitors in BGREF circuitry.
Since analog circuits do not scale very well as technology advances, it is important to develop new architectures which can enable the analog portions to shrink. In addition, the IoT space requires integrated circuits which can operate at different power/performance levels and which are also low cost. The present invention provides novel voltage references which have low area/cost, ultra-low-current and are configurable in terms of their power. The power in the circuit can be easily adjusted over a large range to provide fast wakeup and higher drive currents when needed, and lower current operation for the “always-on” ultra-low power states. The novel circuit concepts can be optimized for the emerging IoT market.
The present invention will be understood and appreciated more fully from the following detailed description taken in conjunction with the drawings in which:
In an embodiment of the present invention, the BGREF includes a switched capacitor (also referred to as switch-cap) circuit.
The impedance Z of a switch-capacitor can be expressed as
where C is the capacitance and s is the frequency. As opposed to resistors, a high impedance switch-cap requires little area, thereby providing a much more compact solution as opposed to the prior art circuitry that uses resistors, which are very large devices in advanced CMOS processes.
The impedance of the switch-cap can be controlled by the frequency (of the switch), and is thus adjustable.
Reference is made to
The non-limiting circuitry of
A capacitor C2 (fixed decoupling capacitor C2) is coupled at one side to an anode and at the other side to a cathode. Two switch capacitor elements SCx and SCy (also referred to as switch capacitor impedance elements), each switch capacitor element including a capacitor C1 coupled with overlapping switches SW1 and SW2, which receive an input frequency from clocks P1 and P2, are each coupled between the anode and cathode in parallel to C2. In SCx, clock P2 is coupled between the anode side of C1 and the anode and the other clock P1 is coupled to the cathode and to the anode side of C1. In SCy, clock P1 is coupled between the anode side of C1 and the anode and the other clock P2 is coupled to the cathode and to the anode side of C1.
Accordingly, there are two non-overlapping switches SW1 and SW2 with frequency inputs from clocks P1 and P2 which are placed in anti-phase over two switched capacitors C1 (also referred to as flying capacitors C1). The capacitors C1 may be, without limitation, metal finger capacitors (MFC), e.g., with a capacitance density of 2 ff/μm2. The fixed decoupling capacitor C2 may be, without limitation, a hybrid gate and metal capacitor, e.g., with a capacitance of 8-10 ff/μm2. C2 is placed there to reduce the ripple caused by the switching action. Note that in
Reference is now made to
A source of PMOS transistor M2B is coupled to a voltage source (Vcc), its drain is coupled to node Vband and its gate is coupled to node PG1. Node PG1 is coupled to the output of an amplifier A1, whose positive input is coupled to Vband and whose negative input is coupled to node Vbe. A source of PMOS transistor M2C is coupled to a voltage source (Vcc), its drain is coupled to node Vbe and its gate is coupled to node PG1.
A switch capacitor element SC1 is coupled at a first terminal (such as, but not necessarily, its anode side) to Vband and at a second terminal (such as, but not necessarily, its cathode side) to a first terminal (such as, but not necessarily, an anode) of a diode D1. The second terminal (such as, but not necessarily, the cathode) of diode D1 is coupled to a negative voltage supply (Vss). A switch capacitor element SC2a is coupled at a first terminal (such as, but not necessarily, its anode side) to Vband and at a second terminal (such as, but not necessarily, its cathode side) to a negative voltage supply (Vss). A switch capacitor element SC2b is coupled at a first terminal (such as, but not necessarily, its anode side) to Vbe and at a second terminal (such as, but not necessarily, its cathode side) to a negative voltage supply (Vss). A first terminal (such as, but not necessarily, an anode) of a diode D2 is coupled to node Vbe and a second terminal (such as, but not necessarily, its cathode) is coupled to a negative voltage supply (Vss). The area ratio of the two diodes is N, which can be, for example, 8 without limitation.
Note that the diode in a more general sense can be any “diode element” which has an electrical behavior similar to a diode. An example of this would be a transistor whose gate is connected to its drain—this type of connection is referred to as a diode-connected device to those skilled in the art. In the case of an NMOS, the gate-drain connection would be the anode, while its source would be the cathode and this would behave like a PN junction diode. In the case of a PMOS, a similar connection would be true; the gate would be connected to the drain, and the gate-drain connection would be the cathode, while the source would be the anode. Thus when we refer to a diode element we mean the generalized definition including a PN junction diode (or parasitic BJT) or the MOS diode-connected devices, and the term “diode” in the specification and claims encompasses such diode elements as well.
A source of PMOS transistor M2A is coupled to a voltage source (Vcc), its drain is coupled to node Vref and its gate is coupled to the gate of M2C. A switch capacitor element SC3 is coupled at its anode side to Vref and at its cathode side to a negative voltage supply (Vss).
Accordingly, the resistors of the prior art circuitry of
It is possible to construct the BGREF circuit with one switch capacitor element and one diode; however, the preferred embodiment has a plurality of switch capacitors and diodes.
In the embodiment of
wherein VT=voltage at a certain absolute temperature T
N=the ratio between the two diodes
SCi=capacitance of the ith switch capacitor
Vbe=base-emitter voltage
The current in the output stage can be expressed as
Iref=Vref*sSC3=s[VT*SC1 ln(N)+SC2*Vbe] (4)
Similarly, the currents in all of the PMOS current sources can be scaled versions of this and are thus highly dependent on the switching frequency and the capacitance values, thereby providing an additional degree of configurability. The voltage can be calibrated by trimming SC3, and the temperature coefficient can be calibrated by trimming SC2(a or b). Since a switch is placed in series with each capacitor element, the trim works by making the switch conducting or non-conducting, such that the capacitance connected to the switch may or may not be connected to the active node of the circuit. Thus the values of C1, C2 and C3 can be controlled digitally by activating these switches and the Vbe, Vref and delta-Vbe terms can each be trimmed independently.
One or all of the capacitors in
The bias for the amplifier in
Reference is now made to
Specifically, the source of an NMOS transistor M1b is coupled to node Vband, and its drain and gate are coupled to node NG1. The source of an NMOS transistor M1c is coupled to node Vbe, its drain is coupled to node PG1 and its gate is coupled to the gate of M1b.
The currents are equal because of the current mirrors M2b and M2c. The voltages at Vband and Vbe are equal due to the source follower action of M1(b,c). In order to improve the gain of the voltage/current mirror circuit, self-biased cascodes may be formed in both M1(b,c) and M2(a,b,c) as shown in the upper left of
The largest flying capacitor of the group may be SC1 since it has the smallest impedance, with a value of ˜0.5-1 pF. The capacitance of SC2(a or b) may be very small, which could result in matching issues. This can be solved by stacking two switch-caps in series and enlarging their size by 233 as shown at SC2a and SC2b in
A comparison of the
The prior art includes:
Y. Osaki, T. Hirose, N. Kuroki and M. Numa, “1.2-V Supply, 100-nW, 1.09-V Bandgap and 0.7-V Supply, 52.5-nW, 0.55-V Subbandgap Reference Circuits for Nanowatt CMOS LSIs,” in IEEE Journal of Solid-State Circuits, vol. 48, no. 6, pp. 1530-1538, June 2013
J. M. Lee, et. al. “A 29 nW Bandgap Reference Circuit”, IEEE ISSCC Dig. Tech. Papers, pp. 100-101, February 2015
Y. Ji et. al. “A 9.3 nW All-in-One Bandgap Voltage and Current Reference Circuit”, IEEE ISSCC Dig. Tech. Papers, pp. 100-101, February 2017
A. Shrivastava, K. Craig, N. E. Roberts, D. D. Wenzloff, and B. H. Calhoun, “A 32 nW Bandgap Reference Voltage Operational from 0.5V Supply for Ultra-Low Power Systems” IEEE ISSCC Dig. Tech. Papers, pp. 94-95, February 2015
Preliminary Results
Simulations of the
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5796313 | Eitan | Aug 1998 | A |
6650594 | Lee | Nov 2003 | B1 |
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