The present invention relates to the field of charge pumps and, more particularly, to methods and circuits for regulating charge pumps.
In many electronic devices, it is desirable to generate a voltage having a magnitude that is greater than a magnitude of a supply voltage providing power to the device. In other applications, it is desirable to generate a polarity that is different from the polarity of the supply voltage providing power to a device. Charge pumps may be used for both of these purposes. Although a wide variety of charge pumps have been developed, many charge pumps use capacitors to obtain a boosted voltage or a voltage having a different polarity.
Typically, a supply voltage is sampled on a first terminal of a capacitor (by charging the capacitor to the supply voltage) during a first phase of a cycle. During a second phase of the cycle, one of the terminals is coupled to a load. If the first terminal of the capacitor is coupled to the load and the second terminal is held at ground, a boosted voltage may be generated. Because the capacitor was charged to the supply voltage during the first phase when the second terminal was connected to ground, the voltage on the first terminal is approximately twice the supply voltage during the second phase. If, during the second phase, the second terminal of the capacitor is coupled to the load and the first terminal is held at ground, a voltage with a reverse polarity may be generated. Because the capacitor was charged to the supply voltage during the first phase when the second terminal was connected to ground, the voltage on the second terminal is approximately a negative supply voltage during the second phase. The charge pump repeatedly alternates between the first and second phases, each cycle generating an output voltage that is approximately twice the supply voltage VAA or of a reversed polarity.
Charge pumps are presently used in a wide variety of applications. For example, charge pumps are typically used in memory devices to provide a negative substrate voltage or to provide a boosted voltage that may be applied to the gate of an NMOS transistor to allow the transistor to couple the supply voltage to an output node. Charge pumps are also used in CMOS imagers to generate voltages of different polarities and magnitudes during various operations carried out by the imagers. For example, charge pumps are commonly used to supply power having a polarity that is different from that of the supply voltage to the imaging array of CMOS imagers.
The time required for a charge pump to output a target voltage is sometimes referred to as a time constant of the charge pump. In general, the time constant of a charge pump driving a resistance load is very short as long as the current demands of the load do not exceed the current that may be supplied by the charge pump. The time constant, however, of a charge pump driving a capacitive load may be very long because the voltage applied to a load incrementally increases through a charge sharing process each cycle. The time constant of the charge pump may affect the magnitude of capacitance relative to the load capacitance, as well as the difference between the supply voltage and the load voltage to which the capacitive load has been charged. The charge pump, thus, may be slow to reach the target voltage because the charge pump may not produce more charge than the combination of the pump capacitance, supply voltage and the load voltage. In addition, charge pumps typically do not compensate for charge lost when the charge pump is inactive.
The invention may be understood from the following detailed description when read in connection with the accompanied drawing. Included in the drawing are the following figures:
Voltage booster circuit 102 includes capacitance Cp, two switches 110, 112 that are closed during the first phase of each cycle and two switches 114, 116 that are closed during the second phase of cycle. Voltage booster circuit 102 may be used to supply a negative voltage when powered by a positive supply voltage 118 of voltage VAA. A load L is connected to output node 126 of charge pump 100. Switches 110, 112 that are closed during the first phase of each cycle are open during the second phase, and switches 114, 116 that are closed during the second phase are open during the first phase. The load L is assumed to be the array of a CMOS imager, which may be highly capacitance, with a capacitance of CL. The voltage across the capacitance load CL is designated as VL. Voltage booster circuit 102 is coupled to voltage regulator circuit 104 via node 128 and switch 114. Voltage booster circuit 102 provides voltage VIN to voltage regulator circuit 104 via node 128 and receives regulator voltage VREG from voltage regulator circuit 104 via switch 114.
Although a capacitive load CL is illustrated in
Voltage regulator circuit 104 includes supply voltage 120 of voltage VAA, capacitor CFB, switches 122, 124 and differential amplifier 108. Switch 122 is closed during the first phase of each cycle and switch 124 is closed during the second phase of each cycle. Switch 122 that is closed during first phase of each cycle is open during the second phase, and switch 124 that is closed during the second phase is open during the first phase. Switch 122 operates together with switch 110, 112 and switch 124 operates in together with switches 114, 116.
Capacitor CFB, switches 122, 124 and supply voltage 120 form level shift circuit 130 that receives voltage VIN from voltage booster circuit 102 generates level shifted voltage VSHIFT. Differential amplifier 108 receives a reference voltage VREF at the non-inverting input terminal and level shifted voltage VSHIFT at the inverting input terminal and produces regulation voltage VREG. Reference voltage VREF represents a target voltage corresponding to a desired negative pumping voltage. Accordingly, to reach an output level of −m volts (where m is an integer), reference voltage VREF can be set at (VAA−m). Capacitor CFB is a feedback capacitor which is used by differential amplifier 108 to detect load voltage VL. In general, capacitor CL is large, for example, 100 times larger, compared to capacitor CP.
As discussed above, in one embodiment, load L may include a diode component, which may introduce a charge leakage to load L. It may be appreciated that the charge leakage may increase exponentially with increasing voltage VL. Accordingly, a threshold voltage for the target voltage (and thus a suitable maxiumum reference voltage VREF) may be determined such that charge pump 100 may compensate for the charge leakage. Charge pump 100, thus, may produce a regulated load voltage VL that may substantially reduce noise due to charge leakage.
During the first phase of each cycle, supply voltage 122 is connected to an upper terminal of capacitor CP by switch 110 while switch 112 connects the lower terminal of capacitor CP to ground. Capacitor CP is therefore charged to −VAA during the first phase. In addition, supply voltage source 120 of voltage regulator circuit 104 is connected to one terminal of capacitor CFB, while switch 112 connects the other terminal of capacitor CFB to ground (i.e., such that VIN is at ground). During the first phase, differential amplifier 108 is disconnected from voltage booster circuit 102 and level shift circuit 102, and capacitors CP and CFB are each charged to VAA.
During the second phase of each cycle, switch 114 is closed to connect the upper terminal of capacitor CP to receive regulation voltage VREG and the other switch 116 is closed to connect the other terminal of capacitor CP to load L. In addition, switch 124 is closed to connect one terminal of capacitor CFB to the inverting input terminal of differential amplifier 108 and the other terminal of CFB is connected to load L and thus to load voltage VL. Thus, a voltage difference of (VAA−VL) is generated across level shift circuit 130.
It may be appreciated that, during the second phase, a feedback circuit is provided by differential amplifier 108 and capacitances CP, CFB. It may also be appreciated that voltage VSHIFT at the inverting input of differential amplifier 108 is at a voltage VAA higher than VL (i.e., it is level shifted). Differential amplifier 108 provides unity gain feedback from VREG to VL. Because of the feedback configuration, differential amplifier 108 adjusts VREG to compensate for any lost charge and to maintain output node 126 at a voltage of VREF−VAA.
In operation, when voltage regulator circuit 104 determines that load voltage VL is outside of a target voltage range, differential amplifier 108 slews to ground (for example, acting as a current sink), such that all charge across CP is pushed into load CL. Accordingly, both output node 126 and level shifted voltage VSHIFT are reduced by ±(CP/CL)·VAA. Thus, the entire supply voltage VAA range is used. When the load voltage VL is within the target voltage range, differential amplifier 108, acting as a voltage buffer, generates regulation voltage VREG to provide sufficient charge into capacitor CP such that the inverting and non-inverting input terminals of differential amplifier 108 are maintained at a substantially same voltage.
By repeating the sequence of first and second phases using a clock, for example, of a few tens of MHz, a large amount of charge may be efficiently moved into capacitor CP while maintaining a smooth settling for the boosted voltage, when the load voltage VL is within the target voltage range. Namely, voltage regulator circuit 104 may 1) rapidly pump load L to within a target voltage range (where differential amplifer 108 acts as a current sink) and 2) apply differential amplifier 108, acting as a voltage buffer, to reach the target voltage. As described further below, a size of capacitor CP, used in charge pump 100, may be reduced. Because the size of capacitor CP may be reduced, a size of an output stage of differential amplifier 108 may also be reduced, thus generating a smaller output current. Accordingly, it may be appreciated that, even with the smaller output current differential amplifier 108 may still be capable of slewing from VAA to ground within a clock phase.
In addition, if differential amplifier 108 has a gain that is fairly high, for example, a gain of greater than 100, voltage booster 102 may keep pumping within the full range (i.e., VAA) until the load voltage VL is within the target voltage range. Because capacitor CP may be charged to supply voltage VAA, a size of capacitor CP may be reduced. Because the output voltage VIN of voltage booster circuit 102 is level shifted by a higher predetermined value (e.g., VAA), voltage booster circuit 102 may be operated using a regulation voltage VREG, which generally produces for a larger voltage (compared to a target voltage) that may be used across capacitor CP. Because a larger voltage may be used in voltage booster circuit 102, a capacitor size needed to reach a target voltage within the time constant may be reduced.
The devices for implementing switches 110, 112, 114, 116, 122, 124 are conventional as are circuitry for controlling them during the first and second phases of each cycle. Therefore, a more detailed explanation of these devices and control circuits have been omitted.
According to another embodiment, charge pumps 100, 200 (
Referring to
As shown in
As described further below, pump clock signals (φ1′, φ2′) are generated to activate and control operation of voltage booster circuit 402 when the load voltage VL at node 434 is less than a reference voltage VREF. When load voltage VL is greater than or equal to reference voltage VREF, pump clock signals (φ1′, φ2′) are set to a low value (i.e. 0) and voltage booster circuit 402 is inactive. Pump clock signals (φ1′, φ2′) represent a first phase (φ1′) and second phase (φ2′) of an active pump cycle.
Voltage booster circuit 402 includes supply voltage 432 of voltage VAA, capacitor CP, two switches 424, 426 that are closed during the first phase (φ1′) of the pump cycle and two switches 428, 430 that are closed during the second phase (®2′) of the pump cycle. Switches 424, 426 that are closed during the first phase of each cycle are open during the second phase. Switches 428, 430 that are closed during the second phase are open during the first phase.
Regulator circuit 404 includes voltage detector circuit 406 and clock generator circuit 408. Voltage detector circuit 406 receives and samples load voltage VL from node 434 and provides a detected voltage VSENSE to clock generator circuit 408. Clock generator circuit 408 generates a set of clock signals (φ1, φ2) to control voltage detector circuit 408 and the set of pump clock signals (φ1′, φ2′) to control voltage booster circuit 402. Clock signals (φ1, φ2) represent a first phase (φ1) and second phase (φ2) of a clock cycle. As described further below, clock signals (φ1, φ2) are generated each clock cycle. Clock signals (φ1′, φ2′), however, are activated when VL is less than reference voltage VREF. Accordingly, regulator circuit 404 detects the load voltage VL and determines whether to activate or deactivate voltage booster circuit 402.
Voltage detector circuit 406 includes capacitor Cs, first set of switches 416, 418 and second set of switches 420, 422. Voltage detector circuit 406 receives and samples load voltage VL on capacitor Cs according to the set of clock signals (φ1, φ2). Switches 416, 418 that are closed during the first phase of each cycle are open during the second phase. Switches 420, 422 that are closed during the second phase of each cycle are open during the first phase. During the second phase, capacitor Cs samples load voltage VL when switches 420, 422 are closed. During the first phase, switches 416, 418 are closed and the detected voltage sampled by capacitor Cs is inverted and provided to clock generator circuit 408 as detected voltage VSENSE.
Clock generator circuit 408 includes comparator 410, clock generator 412 and AND gates 414-1, 414-2. Comparator 410 compares detected voltage VSENSE with reference voltage VREF and generates a pump signal (pump). Comparator 410 generates a high pump signal (i.e., 1) when VSENSE is less than VREF. Comparator 410 generates a low pump signal (i.e., 0) when VSENSE is greater than or equal to VREF. Clock generator 412 generates the set of clock signals φ1, φ2 which is provided to voltage detector circuit 406, regardless of the state of the pump signal. Clock signals φ1, φ2 are gated with the pump signal by AND 414-1, 414-2, respectively, to produce the set of pump clock signals φ1′, φ2′ used to control operation of voltage booster circuit 402. Clock generator circuit 408 sets the set of pump clock signals φ1′, φ2′ to zero when the pump signal is low, thus causing pumping of voltage booster circuit 402 to cease.
Reference voltage VREF represents a target voltage for the load voltage VL at output node 434. Although in one embodiment, VREF is a positive value of 400 mV, it is understood that any suitable reference voltage may be used, based on the load voltage. As described above, load L may also include a diode component that may generate a charge leakage. Accordingly, a suitable VREF may also be based on the charge leakage from the diode component.
In operation, the set of clock signals φ1, φ2 for clock generation circuit 406 continues for each cycle such that voltage detector circuit 406 continually detects load voltage VL. Voltage booster circuit 402, however, is activated when the pump signal is high.
When the pump signal is high and during the second phase of the pump cycle, supply voltage 432 is connected to capacitor CP by switch 430, while switch 428 connects the other terminal of capacitor CP to ground. Capacitor CP is therefore charged to −VAA during the second phase of the pump cycle. During the first phase of the pump cycle, switch 426 is closed to connect the lower terminal of capacitor CP to ground and switch 424 is closed to connect the other terminal of capacitor CP to load L.
In another embodiment, charge pump 400 may include first and second voltage booster circuits 402 (not shown), each connected to regulator circuit 404. The first and second voltage booster circuits 402 are similar to each other except that they are operated out of phase. Accordingly, first and second voltage booster circuits 402 may apply a voltage to load L, as described above, during the first and second phases of each cycle, respectively.
According to one embodiment, when charge pump 400 is used with an imager array, clock generator circuit 408 may be configured with a gate (not shown) to inactivate voltage booster circuit 402 at particular times. In this manner, charge pump 400 may stop pumping, for example, during sampling of a pixel output of imager array to minimize the introduction of switch noise into sampled pixels.
Referring to
To produce the timing diagram shown in
As described above, although a capacitive load CL is shown in
Referring to
As shown in
Although not specifically shown in the drawings, it will be understood that charge pumps 100, 200, 400 or a charge pump according to another example of the invention may be adapted to provide a positive rather than negative load voltage VL. Further, by adding additional switches and a capacitor, charge pumps 100, 200, 400 or a charge pump according to the other example of the invention may generate both positive and negative voltages.
Charge pumps 100, 200, 400 or a charge pump according to some other example of the invention can be used in a wide variety of applications. They are particularly suitable for use in a CMOS imager because the imaging arrays of such devices are highly capacitive (as well as typically including a diode component that may generate a charge leakage). For example, CMOS imager 700 shown in
Although the invention is illustrated and described herein with reference to specific embodiments, the invention is not intended to be limited to the details shown. Rather, various modifications may be made in the details within the scope and range of equivalents of the claims and without departing from the invention.
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