The disclosures herein relate in general to electronic circuitry, and in particular to reducing a settling time after a slew condition in an amplifier.
An amplifier's slew rate is a measure of a maximum rate of change of the amplifier's output voltage in response to an input step function of the amplifier's input voltage. For example, the amplifier's input voltage may be a differential input voltage. A high slew rate is generally desirable.
The amplifier may include a slew boost circuit for: (a) detecting a condition (“slew condition”) in which a threshold difference arises in the differential input voltage; and (b) in response to the slew condition, generating slew current for maintaining the high slew rate. After the slew condition ends (e.g., slew current=0), the amplifier settles various currents and voltages over a period of time (“settling time”) to their usual operating levels. However, in a conventional 3-stage amplifier with the slew boost circuit, the settling time may be unsuitable (e.g., 16-18 bit) for some applications, such as an analog-to-digital converter (“ADC”) driver with high speed and high resolution.
In an amplifier, a first stage receives a differential input voltage, which is formed by first and second input voltages, and outputs a first differential current in response thereto on first and second lines having respective first and second line voltages. A second stage receives the first and second line voltages and outputs a second differential current in response thereto on third and fourth lines having respective third and fourth line voltages. A third stage receives the third and fourth line voltages and outputs an output voltage in response thereto. A slew boost circuit detects a slew condition, in which a threshold difference arises between the first and second input voltages, and outputs a slew current in response thereto for maintaining a slew rate of the output voltage during the slew condition. The first stage includes circuits for reducing a variable difference between the first and second line voltages.
The third stage 106 is a class AB amplifier for generating and outputting an output voltage VOUT on a line LOUT, which is coupled to a voltage reference node VSS (e.g., ground) through an output load 108 whose impedance=ZL. The third stage 106 applies the gain Gm3 to amplify a difference (“ΔV3”) between a line L30's voltage (“V30”) and a line L31's voltage (“V31”). Accordingly, in response to ΔV3, the third stage 106 generates VOUT=ΔV3*Gm3*ZL.
A rate of change of VOUT is dVOUT/dt. The amplifier 100 receives a differential input voltage from lines L10 and L11. The amplifier 100 slew rate is a maximum dVOUT/dt in response to an input step function of the differential input voltage on L10 and L11.
The first stage 102 applies the gain Gm1 to amplify a difference (“ΔVIN”) between L10's voltage (“VIN+”) and L11's voltage (“VIN−”). Accordingly, in response to ΔVIN, the first stage 102 generates a difference (“ΔI2”) between a line L20's current (“I20”) and a line L21's current (“I21”), so that ΔI2=ΔVIN*Gm1. In this example: (a) if ΔVIN is positive, then ΔI2 is negative; and (b) if ΔVIN is negative, then ΔI2 is positive.
The second stage 104 applies the gain Gm2 to amplify a difference (“ΔV2”) between L20's voltage (“V20”) and L21's voltage (“V21”). Accordingly, in response to ΔV2, the second stage 104 generates a difference (“ΔI3”) between L30's current (“I30”) and L31's current (“I31”), so that ΔI3=ΔV2*Gm2. To help stabilize V20, L20 is coupled to VSS through a capacitor C10. Through a first feedback path, Lour is coupled to L21 through a capacitor C11. Through a second feedback path, LOUT is coupled to L30 through a capacitor C2.
If ΔVIN reaches a threshold difference (e.g., 100 mV), then ΔI2 approaches its maximum limit, so that the slew condition occurs. In this example, if ΔVIN is positive while reaching the threshold difference (e.g., VIN+>>VIN−), then the slew condition is positive (“positive slew condition”). Conversely, if ΔVIN is negative while reaching the threshold difference (e.g., VIN+<<VIN−), then the slew condition is negative (“negative slew condition”).
As shown in
ISLEW causes ΔV2 to increase. After the slew condition ends (ISLEW=0), the amplifier 100 reduces ΔV2 over a period of time (“settling time”) to its usual operating level. To reduce the settling time, the first stage 102 operates to constrain ΔV2 during the slew condition, as discussed hereinbelow in connection with
L20 is connected to a collector of an NPN bipolar transistor B0. L21 is connected to a collector of an NPN bipolar transistor B1. Respective emitters of B0 and B1 are connected to VSS. Respective bases of B0 and B1 are connected to one another and are coupled through a current source 204 to VSS, so that: (a) the current source 204 supplies a current for controlling a current mirror that is formed by B0 and B1; and (b) such current mirror operates as a current source.
In the first stage 102, a positive slew boost circuit 206 includes: (a) an n-channel field-effect transistor (“NFET”) N1 whose gate is connected to L20; and (b) an NFET N2 whose gate is connected to L21. Also, the circuit 206 includes a current mirror that is formed by PFETs P1 and P2. Respective sources of P1 and P2 are connected to a voltage supply node VDD. A drain of P1 is connected to respective gates of P1 and P2.
A drain of P2 is connected to a drain of N2 and to a gate of a PFET P3. A source of P3 is connected to L21, and a drain of P3 is connected to VSS. Drains of N1 and N2 are connected to one another and are coupled through current sources 208 and 210 to VSS, so that the current sources 208 and 210 together supply a total current through N1, N2, P1 and P2.
Moreover, in the first stage 102, a negative slew boost circuit 212 includes: (a) an NFET N3 whose gate is connected to L20; and (b) an NFET N4 whose gate is connected to L21. Also, the circuit 206 includes a current mirror that is formed by PFETs P4 and P5. Respective sources of P4 and P5 are connected to VDU. A drain of P4 is connected to respective gates of P4 and P5.
A drain of P5 is connected to a drain of N4 and to a gate of an NFET N5. A source of N5 is connected to L21, and a drain of N5 is connected to VDD, Drains of N3 and N4 are connected to one another and are coupled through current sources 214 and 216 to VSS, so that the current sources 214 and 216 together supply a total current through N3, N4, P4 and P5.
In the positive slew boost circuit 206, its ITOTAL is a sum of currents through the current sources 208 and 210. Similarly, in the negative slew boost circuit 212, its ITOTAL is a sum of currents through the current sources 214 and 216. In a first embodiment: (a) the transistors of the positive slew boost circuit 206 are matched, and its ITOTAL ISLEW; and (b) similarly, the transistors of the negative slew boost circuit 212 are matched, and its ITOTAL ISLEW. Accordingly, in the first embodiment, the positive slew boost circuit 206 and the negative slew boost circuit 212 are shut off in absence of the slew condition (because ISLEW=0 in absence of the slew condition), which conserves power.
In a second embodiment, the transistors of the positive slew boost circuit 206 are intentionally mismatched, and the transistors of the negative slew boost circuit 212 are intentionally mismatched, which allows for easier implementation. In a first version of such embodiment, ITOTAL≈ISLEW. In a second version of such embodiment, ITOTAL√ICONST, where ICONST is a relatively constant current. In a third version of such embodiment, ITOTAL≈ISLEW+ICONST.
In the first stage 102 operation, if ΔVIN is a positive difference (VIN+>VIN−), then less current from the source 202 flows through P10 and B0, and more current from the source 202 flows through P11 and B1 Conversely, if ΔVIN is a negative difference (VIN+<VIN−), then more current from the source 202 flows through P10 and B0, and less current from the source 202 flows through P11 and B1.
Positive slew boost refers to the positive slew condition, in which VIN+>VIN−, so that V20<V21. In the positive slew condition, the positive slew boost circuit 206 lowers V21 to constrain ΔV2 near its usual operating level. For example, as ISLEW causes V20<V21, more current flows through N2, because L21 is connected to the gate of N2.
As more current flows through N2, its drain voltage is lowered. As N2's drain voltage is lowered, more current flows through P3, because N2's drain is connected to the gate of P3. As more current flows through P3: (a) its source voltage is lowered; and (b) likewise, V21 is lowered, because L21 is connected to the source of P3. This cycle progressively repeats until eventually: (a) current through P2 and N2 becomes substantially balanced with current through P1 and N1 (which is controlled by V20 at the gate of N1); and (b) accordingly, V21 becomes approximately equal to V20, so that the positive slew boost circuit 206 thereby constrains ΔV2 near its usual operating level.
Negative slew boost refers to the negative slew condition, in which VIN+<VIN−, so that V20>V21. In the negative slew condition, the negative slew boost circuit 212 raises V21 to constrain ΔV2 near its usual operating level. For example, as ISLEW causes V20>V21, less current flows through N4, because L21 is connected to the gate of N4.
As less current flows through N4, its drain voltage is raised. As N4's drain voltage is raised, more current flows through N5, because N4's drain is connected to the gate of N5. As more current flows through N5: (a) its source voltage is raised; and (b) likewise, V21 is raised, because L21 is connected to the source of N5. This cycle progressively repeats until eventually: (a) current through P5 and N4 becomes substantially balanced with current through P4 and N3 (which is controlled by V20 at the gate of N3); and (b) accordingly, V21 becomes approximately equal to V20, so that the negative slew boost circuit 212 thereby constrains ΔV2 near its usual operating level.
In that manner, despite the positive or negative slew condition, the first stage 102 constrains ΔV2 near its usual operating level. After the slew condition ends (ISLEW=0), the first stage 102 quickly settles V20 and V21 to their usual operating levels, because the amplifier 100 feedback quickly corrects for any remaining error. Accordingly: (a) in response to detecting the slew condition, the amplifier 100 generates slew current to maintain a high slew rate with class AB output; (b) ΔV2 is inherently stable before, during and after the slew condition; (c) the amplifier 100 has a relatively low settling time after the slew condition ends; and (d) the amplifier 100 consumes relatively low power (e.g., <10 nA).
By comparison, if a diode is placed between L20 and L21 to restrict a maximum difference between V20 and V21 during the slew condition, then the diode would have a voltage drop (e.g., 0.7 v). Such voltage drop would increase the amplifier 100 settling time after the slew condition ends.
Although illustrative embodiments have been shown and described by way of example, a wide range of alternative embodiments is possible within the scope of the foregoing disclosure.
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