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An Analog CMOS Double-Edge Multi-Phase Low-
Latency Pulse Width Modulator
Jianhui Zhang Seth R. Sanders
University of California, Berkeley
Berkeley, CA 94720 USA
zhangjh, sanders@eecs.berkeley.edu
Abstract-This paper presents an analog CMOS double-edge
multi-phase low-latency pulse width modulator. The PWM
signal is generated by comparing the phase difference between
two matched ring oscillators, which are differentially driven by
the command voltage and the feedback voltage developed in a
minor loop that forces the average frequency of each of the
oscillators to be equal. Both rising and falling edges of the PWM
signal are controlled by the instantaneous input voltage,
resulting in a low latency relative to that achieved with
conventional latched PWM circuitry. The developed pulse width
modulator has high precision, good linearity, good noise
immunity and wide duty ratio range. Further, it can be flexibly
reconfigured for multi-phase PWM operation with no restriction
on duty cycle range. The complete double-edge pulse width
modulator IC is implemented in a 0.18 gm CMOS process. It can
generate as many as sixteen PWM outputs. The active chip area
is 0.04 mm2. The quiescent bias current of the chip is 80 jA at
1.2 MHz PWM frequency.
I. INTRODUCTION
A multi-phase double-edge pulse width modulation (PWM)
scheme with low latency is important for achieving fast
controller response for high bandwidth applications, such as
those arising in applications like microprocessor voltage
regulator modules [1] or dynamic power supplies for RF
power amplifiers [2]. Although, the required functionality
might be realized with a conventional ramp-comparator
modulator, such a modulator imposes a maximum duty cycle
of 1/N, where N is the number of phases. Another
embodiment of the conventional ramp-comparator modulator
to realize multi-phase operation without the duty cycle
constraint requires N comparators and N uniformly skewed
ramp signals. The modulator described in this paper realizes
all the desired features in a single simple circuit cell.
This paper presents an analog multi-phase double-edge
pulse width modulator suitable for implementation in CMOS
technology. The PWM signal is generated by comparing the
phase difference between two matched ring oscillators, each
of which functions as a current-controlled oscillator. These
two matched oscillators are fed by the currents developed in a
differential input stage. This balanced input stage is driven by
the command voltage waveform, and a feedback voltage
developed in a minor loop that forces the average frequency
of each of the current-controlled ring oscillators to be equal.
The minor loop constrains the duty ratio of the PWM signal to
be proportional to the input modulation voltage over the full
bandwidth of the minor loop. Both rising and falling edges of
the PWM signal are controlled by the instantaneous input
voltage, resulting in a low latency relative to that achieved
with conventional latched PWM circuitry. The developed
pulse width modulator has high precision, good linearity,
good noise immunity and wide duty ratio range. Further, it
can be flexibly reconfigured for multi-phase PWM operation
with no restriction on duty cycle range.
II. CONCEPT OF OPERATION
A simplified schematic of the ring-oscillator-based pulse-
width modulator is shown in Fig. 1. A matched pair MPI-MP2
drives two identical ring oscillators as a matched load. As
illustrated in Fig. 1(b), the phase difference of the two
oscillators is detected by a phase comparator, the output of
which is used as the PWM signal. This phase-sensitive signal
is then passed through a low pass filter (LPF), aimed at
removing ripple, with the resulting signal VFB applied to the
differential pair in an internal feedback loop. In steady state,
the voltage VFB which is proportional to the duty cycle, is
forced to be equal to the command voltage Vin by the minor
feedback loop. When the command modulation voltage Vin
increases, the error voltage between Vin and VFB develops
differential current in the two ring oscillators that results in
instantaneous differential frequency and phase shift as shown
in Fig. l(c). The resulting phase difference of the two ring
oscillators is increased until the signals Vin and VFB are equal.
When the command modulation voltage Vin decreases, as
shown in Fig. l(d), the phase difference of the two ring
oscillators is decreased until the voltages Vin and VFB are
equal. As both edges of the output PWM signal are modulated
by the input command voltage Vin, the behavior of this ring-
oscillator-based pulse width modulator is similar to a double-
edge PWM modulator. The phase difference of two ring
oscillators is actually equal to the time integral of the
differences of the two ring oscillator frequencies, which is
proportional to the error voltage. Therefore, integration
inherently takes place in the loop and any high frequency
noise or glitch at the input is filtered, suppressing false
transitions. Instead of comparing the phase difference once
per switching period, M uniformly spaced taps on each
respective ring oscillator are compared in a multi-phase phase
comparator, reducing latency and increasing the phase
comparator ripple frequency. Further, uniformly spaced
1-4244-0714-1/07/$20.00 C 2007 IEEE. 355
VDD
OFB
(a)
(b)BCrn
O'
IC)
VPWM-Jffi§-JL
(di)
Figure 1. (a) Simplified schematic of ring-oscillator-based pulse-width modulator (b) Steady state switching waveforms (c) Switching waveforms as input control
voltage increases (d) Switching waveforms as input control voltage decreases.
multi-phase PWM signals are available from the multi-phase
phase comparator. A multi-input low pass filter is applied to
suppress ripple in the minor loop.
Ignoring the nonlinearity of the input differential pair and
phase comparator, a linear model representing the ring-
oscillator-based pulse-width modulator is shown in Fig. 2.
This model consists of the input differential pair with
transconductance Gm, the phase comparator modeled as a gain
term KPD, the low pass filter (LPF) with -3dB frequency OLPF;
the buffer with voltage swing of VDD to drive the low pass
filter; and the current-starved ring oscillator modeled as an
integrator 1/S with the gain Kosc [3]. The closed-loop transfer
function of the pulse-width modulator is given by
D KOSCKPDGm(S + LPF) (1)
Vin s2 + )LPFS+ KOSCKpDSGmVDD )LPF
This corresponds to a second-order feedback loop with two
open-loop poles given by p1 = 0 and P2 = COLPF. As the loop
gain further increases, the two poles become complex with
real part equal to -WLpF/2 and move parallel to the jco-axis. The
loop gain, which is equal to KoscKPDGmVDD, is designed such
that the loop has large bandwidth for fast dynamic response
and enough phase margin so as not to cause significant
overshoot in the step response. Since there is one open-loop
pole at the origin, the loop gain goes to infinity as s - 0 which
ensures that the error voltage goes to zero in steady state. In
equation 1, by making s - 0, the duty cycle of the pulse width
modulator output is given by
D=Vin/VDD (2)
which is proportional to the input control voltage Vin.
Difl. Pair Ring Osc. Phase Comp.
Vlr VPWM
Figure 2. Linear model ofthe ring-oscillator based pulse-width modulator
III. CIRCUIT IMPLEMENTATION
A. Input Stage
The input stage compares the voltage difference between
the command Vin and the feedback voltage VFB, and converts
voltage into current to bias the ring oscillators. There are
several design considerations regarding the input stage of this
ring-oscillator-based pulse-width modulator. First, the input
stage should not saturate with large differential voltage as
saturation would significantly limit the transient response of
the modulator. Second, the transconductance of the input
stage should be large enough to achieve the desired loop
bandwidth, and be well controlled to keep good phase margin.
Finally, the quiescent current supplied to the ring oscillator
must be well controlled as it determines the nominal ring
oscillator frequency, which is the same as the PWM switching
frequency. Based on the above considerations, common-
source transistor Mp1 and MP2 together with a pre-amplifier [4]
are used as the input stage, as shown in Fig. 3(a). The whole
input stage is symmetric and Fig. 3(b) shows half of the
356
VDD
r-
mpi P2
i
V.
Pre-Amplifer
To Ring Oscillators
(a)
Pre-Amplifier
(b)
Figure 3. (a) Simplified schematic of the input stage (b) Half-circuit of the
pre-amplifier.
circuit. The error voltage at the input is sensed by differential
pair M1 and M2, which is biased by the tail current source 12.
Common drain transistors M5 and M6 are in parallel with the
current mirror load M3 and M4 to reduce the output resistance
so that the gain of the error amplifier can be set to a well-
defined value. The negative feedback loop, including
transistors M3, M5, M7 and current source I1, adjusts the gate
voltage of M5 such that M7 operates in the active region and
conducts I1. It can be shown that the quiescent bias current of
Mp1 is given by
IDP = I1 (W/L)pI (3)D
'PII(WI/L)7
and the overall transconductance of the input stage is
Gm = gm,MP1 (4)
9m6
Compared to the conventional differential pair, this input
stage provides a large relative constant transconductance over
a wide range of differential input voltage, and the quiescent
bias current of Mp1 can be precisely controlled by current
source I1.
B. Ring Oscillator
Figure 4. Simplified schematic of the ring oscillator
A current starved differential ring oscillator similar to the
design in [5] is used here for its small area and low power
consumption. As shown in Fig. 4, the supply current to the
ring oscillator is generated by the common source transistor
Mp1 from the input stage. The differential delay buffer in the
ring oscillator is a pair of inverters with outputs coupled by
weak cross-coupled inverters, aiming at minimizing the delay
skew between two paths. The voltage swing on the ring
oscillator is below the threshold of the MOSFET, which gives
the ring oscillator a good linear dependency of the oscillation
frequency on the supply current [5].
C. Phase Comparator
The phase comparator compares the phase difference of the
two ring oscillators and the PWM signal is taken from the
output. The phase comparator is designed to have comparison
range from 0 to 27r, linearly corresponding to 0 to 100% duty
ratio. When the instantaneous phase difference exceeds the 0
to 27r range, the duty cycle should saturate to 0 or 100% to
avoid wind-up. The problem with this saturating phase
detection scheme is that the frequency of the two oscillators
will lose lock if the phase difference exceeds the 0 to 27t range,
as more feedback voltage will have to be applied to the input
differential pair in order for the oscillator phase to shift
accordingly. However, the phase comparator can produce no
more dc output voltage to shift the oscillator frequency further,
as the duty ratio reaches 0 or 100%, so the loop will lose lock.
To resolve this frequency tracking problem, a phase and
frequency detection scheme is developed as shown in Fig.
5(a). A phase-frequency comparator compares the phase and
frequency difference of two ring oscillators, and the PWVM
signal is taken from the output. Instead of feeding back the
DC component of the PWM signal, a four level signal Vit as
shown in Fig. 5(b) is developed from the phase comparator to
close the internal feedback loop. When the phase difference is
within 0 to 27t range, VLP swings between VL and VH, linearly
corresponding to 0 to 100% duty ratio. When the phase
difference becomes negative, VLP swings between 0 and VL,
providing extra voltage to pull the phase difference of the two
357
VIP
(Ia)
CA
Out ]
......VDD
.....VH
v;. nF VLt
LJ ..L J ~........................... 0
(b)
Figure 5. Proposed phase frequency detection scheme.
Reset
(0
I B
ALdA
I(OB
I (A
State
ID10j
Figure 6. State transition diagram of the phase frequency comparator state
machine.
ring oscillators back to zero and keep the loop locked. An
analogous case applies when phase difference exceeds 27t,
VLP swings between VH and VDD, providing extra voltage
room on the feedback node to keep the loop in lock.
The proposed phase and frequency detection scheme is
implemented by using a state machine with the state transition
diagram shown in Fig. 6. A state transition occurs only when
the rising edge of either one of the frequency inputs is
detected by the phase comparator. When the phase difference
is within the normal 0 to 27r range, transitions only occur
between states S1 and S2. When the state machine receives
two consecutive rising edges from either one of the frequency
inputs, meaning the phase difference exceeds the 0 to 27t
range, the state machine will transition to a saturation state,
with So and S3 coffesponding to the case of phase difference
Figure 7. Chip micrograph.
Figure 8. Four symmetric PWM output signals
below 0 or above 27t, respectively. The PWM signal is taken
by combining the two bits of the state in a XNOR gate. A set
of M such phase frequency comparators are used to compare
all the taps from two ring oscillators to reduce the latency. A
multi-input low pass filter is used to reduce the ripple voltage
and increase the loop bandwidth.
IV. EXPREIMENTAL RESULTS
The complete double-edge pulse width modulator IC is
implemented in a 0.18 ltm CMOS process. The die photo of
the chip is shown in Fig. 7. The active chip area is 0.04 mm2.
It can generate as many as sixteen PWM outputs. Fig. 8
shows four of sixteen symmetric PWM output signals. The
quiescent bias current of the chip is 80 iA at 1.2 MHz PWM
frequency, and much higher PWM frequency is possible by
358
400 nsdvsd
o00
90
80
70
60
0
40
3020
10
0.) 0.6 0. 7 0 .9 1 1. 1.
Input Modulation Voltage Vin (V)
Duty rati to 1000
Vin
DuLty ratio s awrates t'o 0 - ~
PWM
2 -us/div
(b)
Figure 9. Experimental time domain response of the modulator to a triangle
input voltage (a) no duty ratio saturation (b) with duty ratio saturates to both
0 and 100%.
increasing the bias current of the ring oscillator.
Fig. 9(a) shows the time domain response of the modulator
to a triangle input voltage command Vin without duty ratio
saturation. The functionality of the proposed phase
comparator is verified by applying a large triangle voltage
command Vin at the input and forcing the duty ratio of the
PWM signal to saturate to zero and 100%. Fig. 9(b) shows the
corresponding time domain response of the modulator output.
The modulator is able to generate PWM signal with zero and
100% duty ratio and recover from each saturation state to
normal operation. Fig. 10 gives the measured output PWM
duty ratio versus input voltage command Vin, showing the
good linearity of the pulse-width modulator. The low-latency
double-edge modulation characteristic is verified by applying
a large step voltage at the input. A negative step input voltage
Figure 10. Measured transfer characteristic of PWM duty ratio versus input
voltage.
and two of the sixteen PWM output signals (with 180 degree
phase shift) are shown in Fig. 11 (a). The period of the PWM
signal is approximate 880ns. The falling edge of PWM2 is
generated right after applying the voltage step at the input
with 60ns delay. The response to a positive step input voltage
is shown in Fig. 11 (b). The rising edge of PWM2 is generated
right after applying the voltage step at the input with 60ns
delay. As seen, both edges of the PWM signal are modulated
by the input voltage and the designed PWM modulator
provides fast transient response.
V. CONCLUSION
A CMOS double-edge pulse-width modulator has been
demonstrated in this paper. The PWM signal is generated by
comparing the phase difference between two ring oscillators,
which are driven by the input command voltage and a
feedback voltage developed in a minor feedback loop that
forces the average frequency of the two oscillators to be equal.
A multi-state phase frequency detection scheme is developed
to keep the frequency of two oscillators always in lock. Both
rising and falling edge of the PWM signal are controlled by
the instantaneous input voltage, resulting in a low latency
relative to that achieved with conventional PWM circuitry.
The fast transient response, good re-configurability, good
linearity and noise immunity, low power and low cost make it
an attractive pulse width modulator candidate for integrated
power management ICs.
359
(a)
0
1-1
0.,-.4
1.
P4
-4-i
gl-.
vin
PWMI
PWM2 60ns 400ns/div
[1] A. V. Peterchev and S. R. Sanders, "Design of ceramic-capacitor
VRM's with estimated load current feedforward," in Proc. IEEE Power
Electron. Spec. Conf., 2004, pp. 4325-4332.
[2] G. Hanington, P.F.Chen, P.Asbeck, and L.E.Larson, "High-efficiency
power amplifier using power supply voltage for CDMA applications,"
IEEE Transactions on Microwave theory and Techniques, vol. 47, pp.
1471-1476, August 1999.
[3] P. R. Gray, P. J. Hurst, S.H. Lewis, and R. G. Meyer, Analysis and
Design ofAnalog Integrated Circuits, 4th ed. New York: Wiely, 2001.
[4] H. Khorramabadi, "A CMOS line driver with 90db linearity for ISDN
application," IEEE Journal ofSolid-Stage Circuits, vol. 27, pp. 539-544,
April 1992.
[5] J. Xiao, A. V. Peterchev, J. Zhang, and S. R. Sanders, "A 4 pA
quiescent current dual-mode digitally controlled buck converter IC for
cellular phone applications," IEEE Journal of Solid-Stage Circuits, vol.
39, no. 12, pp. 2342-2348, December 2004.
(a)
Vin
PWMI
PWM2
,60ns 4OQns/div
(b)
Figure 11. Experimental transient response of the pulse-width modulator (a)
applying step down voltage at input (b) applying step up voltage at input.
360
REFERENCES

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Analog CMOS Double-Edge Multi-Phase Low-Latency PWM

  • 1. An Analog CMOS Double-Edge Multi-Phase Low- Latency Pulse Width Modulator Jianhui Zhang Seth R. Sanders University of California, Berkeley Berkeley, CA 94720 USA zhangjh, sanders@eecs.berkeley.edu Abstract-This paper presents an analog CMOS double-edge multi-phase low-latency pulse width modulator. The PWM signal is generated by comparing the phase difference between two matched ring oscillators, which are differentially driven by the command voltage and the feedback voltage developed in a minor loop that forces the average frequency of each of the oscillators to be equal. Both rising and falling edges of the PWM signal are controlled by the instantaneous input voltage, resulting in a low latency relative to that achieved with conventional latched PWM circuitry. The developed pulse width modulator has high precision, good linearity, good noise immunity and wide duty ratio range. Further, it can be flexibly reconfigured for multi-phase PWM operation with no restriction on duty cycle range. The complete double-edge pulse width modulator IC is implemented in a 0.18 gm CMOS process. It can generate as many as sixteen PWM outputs. The active chip area is 0.04 mm2. The quiescent bias current of the chip is 80 jA at 1.2 MHz PWM frequency. I. INTRODUCTION A multi-phase double-edge pulse width modulation (PWM) scheme with low latency is important for achieving fast controller response for high bandwidth applications, such as those arising in applications like microprocessor voltage regulator modules [1] or dynamic power supplies for RF power amplifiers [2]. Although, the required functionality might be realized with a conventional ramp-comparator modulator, such a modulator imposes a maximum duty cycle of 1/N, where N is the number of phases. Another embodiment of the conventional ramp-comparator modulator to realize multi-phase operation without the duty cycle constraint requires N comparators and N uniformly skewed ramp signals. The modulator described in this paper realizes all the desired features in a single simple circuit cell. This paper presents an analog multi-phase double-edge pulse width modulator suitable for implementation in CMOS technology. The PWM signal is generated by comparing the phase difference between two matched ring oscillators, each of which functions as a current-controlled oscillator. These two matched oscillators are fed by the currents developed in a differential input stage. This balanced input stage is driven by the command voltage waveform, and a feedback voltage developed in a minor loop that forces the average frequency of each of the current-controlled ring oscillators to be equal. The minor loop constrains the duty ratio of the PWM signal to be proportional to the input modulation voltage over the full bandwidth of the minor loop. Both rising and falling edges of the PWM signal are controlled by the instantaneous input voltage, resulting in a low latency relative to that achieved with conventional latched PWM circuitry. The developed pulse width modulator has high precision, good linearity, good noise immunity and wide duty ratio range. Further, it can be flexibly reconfigured for multi-phase PWM operation with no restriction on duty cycle range. II. CONCEPT OF OPERATION A simplified schematic of the ring-oscillator-based pulse- width modulator is shown in Fig. 1. A matched pair MPI-MP2 drives two identical ring oscillators as a matched load. As illustrated in Fig. 1(b), the phase difference of the two oscillators is detected by a phase comparator, the output of which is used as the PWM signal. This phase-sensitive signal is then passed through a low pass filter (LPF), aimed at removing ripple, with the resulting signal VFB applied to the differential pair in an internal feedback loop. In steady state, the voltage VFB which is proportional to the duty cycle, is forced to be equal to the command voltage Vin by the minor feedback loop. When the command modulation voltage Vin increases, the error voltage between Vin and VFB develops differential current in the two ring oscillators that results in instantaneous differential frequency and phase shift as shown in Fig. l(c). The resulting phase difference of the two ring oscillators is increased until the signals Vin and VFB are equal. When the command modulation voltage Vin decreases, as shown in Fig. l(d), the phase difference of the two ring oscillators is decreased until the voltages Vin and VFB are equal. As both edges of the output PWM signal are modulated by the input command voltage Vin, the behavior of this ring- oscillator-based pulse width modulator is similar to a double- edge PWM modulator. The phase difference of two ring oscillators is actually equal to the time integral of the differences of the two ring oscillator frequencies, which is proportional to the error voltage. Therefore, integration inherently takes place in the loop and any high frequency noise or glitch at the input is filtered, suppressing false transitions. Instead of comparing the phase difference once per switching period, M uniformly spaced taps on each respective ring oscillator are compared in a multi-phase phase comparator, reducing latency and increasing the phase comparator ripple frequency. Further, uniformly spaced 1-4244-0714-1/07/$20.00 C 2007 IEEE. 355
  • 2. VDD OFB (a) (b)BCrn O' IC) VPWM-Jffi§-JL (di) Figure 1. (a) Simplified schematic of ring-oscillator-based pulse-width modulator (b) Steady state switching waveforms (c) Switching waveforms as input control voltage increases (d) Switching waveforms as input control voltage decreases. multi-phase PWM signals are available from the multi-phase phase comparator. A multi-input low pass filter is applied to suppress ripple in the minor loop. Ignoring the nonlinearity of the input differential pair and phase comparator, a linear model representing the ring- oscillator-based pulse-width modulator is shown in Fig. 2. This model consists of the input differential pair with transconductance Gm, the phase comparator modeled as a gain term KPD, the low pass filter (LPF) with -3dB frequency OLPF; the buffer with voltage swing of VDD to drive the low pass filter; and the current-starved ring oscillator modeled as an integrator 1/S with the gain Kosc [3]. The closed-loop transfer function of the pulse-width modulator is given by D KOSCKPDGm(S + LPF) (1) Vin s2 + )LPFS+ KOSCKpDSGmVDD )LPF This corresponds to a second-order feedback loop with two open-loop poles given by p1 = 0 and P2 = COLPF. As the loop gain further increases, the two poles become complex with real part equal to -WLpF/2 and move parallel to the jco-axis. The loop gain, which is equal to KoscKPDGmVDD, is designed such that the loop has large bandwidth for fast dynamic response and enough phase margin so as not to cause significant overshoot in the step response. Since there is one open-loop pole at the origin, the loop gain goes to infinity as s - 0 which ensures that the error voltage goes to zero in steady state. In equation 1, by making s - 0, the duty cycle of the pulse width modulator output is given by D=Vin/VDD (2) which is proportional to the input control voltage Vin. Difl. Pair Ring Osc. Phase Comp. Vlr VPWM Figure 2. Linear model ofthe ring-oscillator based pulse-width modulator III. CIRCUIT IMPLEMENTATION A. Input Stage The input stage compares the voltage difference between the command Vin and the feedback voltage VFB, and converts voltage into current to bias the ring oscillators. There are several design considerations regarding the input stage of this ring-oscillator-based pulse-width modulator. First, the input stage should not saturate with large differential voltage as saturation would significantly limit the transient response of the modulator. Second, the transconductance of the input stage should be large enough to achieve the desired loop bandwidth, and be well controlled to keep good phase margin. Finally, the quiescent current supplied to the ring oscillator must be well controlled as it determines the nominal ring oscillator frequency, which is the same as the PWM switching frequency. Based on the above considerations, common- source transistor Mp1 and MP2 together with a pre-amplifier [4] are used as the input stage, as shown in Fig. 3(a). The whole input stage is symmetric and Fig. 3(b) shows half of the 356
  • 3. VDD r- mpi P2 i V. Pre-Amplifer To Ring Oscillators (a) Pre-Amplifier (b) Figure 3. (a) Simplified schematic of the input stage (b) Half-circuit of the pre-amplifier. circuit. The error voltage at the input is sensed by differential pair M1 and M2, which is biased by the tail current source 12. Common drain transistors M5 and M6 are in parallel with the current mirror load M3 and M4 to reduce the output resistance so that the gain of the error amplifier can be set to a well- defined value. The negative feedback loop, including transistors M3, M5, M7 and current source I1, adjusts the gate voltage of M5 such that M7 operates in the active region and conducts I1. It can be shown that the quiescent bias current of Mp1 is given by IDP = I1 (W/L)pI (3)D 'PII(WI/L)7 and the overall transconductance of the input stage is Gm = gm,MP1 (4) 9m6 Compared to the conventional differential pair, this input stage provides a large relative constant transconductance over a wide range of differential input voltage, and the quiescent bias current of Mp1 can be precisely controlled by current source I1. B. Ring Oscillator Figure 4. Simplified schematic of the ring oscillator A current starved differential ring oscillator similar to the design in [5] is used here for its small area and low power consumption. As shown in Fig. 4, the supply current to the ring oscillator is generated by the common source transistor Mp1 from the input stage. The differential delay buffer in the ring oscillator is a pair of inverters with outputs coupled by weak cross-coupled inverters, aiming at minimizing the delay skew between two paths. The voltage swing on the ring oscillator is below the threshold of the MOSFET, which gives the ring oscillator a good linear dependency of the oscillation frequency on the supply current [5]. C. Phase Comparator The phase comparator compares the phase difference of the two ring oscillators and the PWM signal is taken from the output. The phase comparator is designed to have comparison range from 0 to 27r, linearly corresponding to 0 to 100% duty ratio. When the instantaneous phase difference exceeds the 0 to 27r range, the duty cycle should saturate to 0 or 100% to avoid wind-up. The problem with this saturating phase detection scheme is that the frequency of the two oscillators will lose lock if the phase difference exceeds the 0 to 27t range, as more feedback voltage will have to be applied to the input differential pair in order for the oscillator phase to shift accordingly. However, the phase comparator can produce no more dc output voltage to shift the oscillator frequency further, as the duty ratio reaches 0 or 100%, so the loop will lose lock. To resolve this frequency tracking problem, a phase and frequency detection scheme is developed as shown in Fig. 5(a). A phase-frequency comparator compares the phase and frequency difference of two ring oscillators, and the PWVM signal is taken from the output. Instead of feeding back the DC component of the PWM signal, a four level signal Vit as shown in Fig. 5(b) is developed from the phase comparator to close the internal feedback loop. When the phase difference is within 0 to 27t range, VLP swings between VL and VH, linearly corresponding to 0 to 100% duty ratio. When the phase difference becomes negative, VLP swings between 0 and VL, providing extra voltage to pull the phase difference of the two 357
  • 4. VIP (Ia) CA Out ] ......VDD .....VH v;. nF VLt LJ ..L J ~........................... 0 (b) Figure 5. Proposed phase frequency detection scheme. Reset (0 I B ALdA I(OB I (A State ID10j Figure 6. State transition diagram of the phase frequency comparator state machine. ring oscillators back to zero and keep the loop locked. An analogous case applies when phase difference exceeds 27t, VLP swings between VH and VDD, providing extra voltage room on the feedback node to keep the loop in lock. The proposed phase and frequency detection scheme is implemented by using a state machine with the state transition diagram shown in Fig. 6. A state transition occurs only when the rising edge of either one of the frequency inputs is detected by the phase comparator. When the phase difference is within the normal 0 to 27r range, transitions only occur between states S1 and S2. When the state machine receives two consecutive rising edges from either one of the frequency inputs, meaning the phase difference exceeds the 0 to 27t range, the state machine will transition to a saturation state, with So and S3 coffesponding to the case of phase difference Figure 7. Chip micrograph. Figure 8. Four symmetric PWM output signals below 0 or above 27t, respectively. The PWM signal is taken by combining the two bits of the state in a XNOR gate. A set of M such phase frequency comparators are used to compare all the taps from two ring oscillators to reduce the latency. A multi-input low pass filter is used to reduce the ripple voltage and increase the loop bandwidth. IV. EXPREIMENTAL RESULTS The complete double-edge pulse width modulator IC is implemented in a 0.18 ltm CMOS process. The die photo of the chip is shown in Fig. 7. The active chip area is 0.04 mm2. It can generate as many as sixteen PWM outputs. Fig. 8 shows four of sixteen symmetric PWM output signals. The quiescent bias current of the chip is 80 iA at 1.2 MHz PWM frequency, and much higher PWM frequency is possible by 358 400 nsdvsd
  • 5. o00 90 80 70 60 0 40 3020 10 0.) 0.6 0. 7 0 .9 1 1. 1. Input Modulation Voltage Vin (V) Duty rati to 1000 Vin DuLty ratio s awrates t'o 0 - ~ PWM 2 -us/div (b) Figure 9. Experimental time domain response of the modulator to a triangle input voltage (a) no duty ratio saturation (b) with duty ratio saturates to both 0 and 100%. increasing the bias current of the ring oscillator. Fig. 9(a) shows the time domain response of the modulator to a triangle input voltage command Vin without duty ratio saturation. The functionality of the proposed phase comparator is verified by applying a large triangle voltage command Vin at the input and forcing the duty ratio of the PWM signal to saturate to zero and 100%. Fig. 9(b) shows the corresponding time domain response of the modulator output. The modulator is able to generate PWM signal with zero and 100% duty ratio and recover from each saturation state to normal operation. Fig. 10 gives the measured output PWM duty ratio versus input voltage command Vin, showing the good linearity of the pulse-width modulator. The low-latency double-edge modulation characteristic is verified by applying a large step voltage at the input. A negative step input voltage Figure 10. Measured transfer characteristic of PWM duty ratio versus input voltage. and two of the sixteen PWM output signals (with 180 degree phase shift) are shown in Fig. 11 (a). The period of the PWM signal is approximate 880ns. The falling edge of PWM2 is generated right after applying the voltage step at the input with 60ns delay. The response to a positive step input voltage is shown in Fig. 11 (b). The rising edge of PWM2 is generated right after applying the voltage step at the input with 60ns delay. As seen, both edges of the PWM signal are modulated by the input voltage and the designed PWM modulator provides fast transient response. V. CONCLUSION A CMOS double-edge pulse-width modulator has been demonstrated in this paper. The PWM signal is generated by comparing the phase difference between two ring oscillators, which are driven by the input command voltage and a feedback voltage developed in a minor feedback loop that forces the average frequency of the two oscillators to be equal. A multi-state phase frequency detection scheme is developed to keep the frequency of two oscillators always in lock. Both rising and falling edge of the PWM signal are controlled by the instantaneous input voltage, resulting in a low latency relative to that achieved with conventional PWM circuitry. The fast transient response, good re-configurability, good linearity and noise immunity, low power and low cost make it an attractive pulse width modulator candidate for integrated power management ICs. 359 (a) 0 1-1 0.,-.4 1. P4 -4-i gl-.
  • 6. vin PWMI PWM2 60ns 400ns/div [1] A. V. Peterchev and S. R. Sanders, "Design of ceramic-capacitor VRM's with estimated load current feedforward," in Proc. IEEE Power Electron. Spec. Conf., 2004, pp. 4325-4332. [2] G. Hanington, P.F.Chen, P.Asbeck, and L.E.Larson, "High-efficiency power amplifier using power supply voltage for CDMA applications," IEEE Transactions on Microwave theory and Techniques, vol. 47, pp. 1471-1476, August 1999. [3] P. R. Gray, P. J. Hurst, S.H. Lewis, and R. G. Meyer, Analysis and Design ofAnalog Integrated Circuits, 4th ed. New York: Wiely, 2001. [4] H. Khorramabadi, "A CMOS line driver with 90db linearity for ISDN application," IEEE Journal ofSolid-Stage Circuits, vol. 27, pp. 539-544, April 1992. [5] J. Xiao, A. V. Peterchev, J. Zhang, and S. R. Sanders, "A 4 pA quiescent current dual-mode digitally controlled buck converter IC for cellular phone applications," IEEE Journal of Solid-Stage Circuits, vol. 39, no. 12, pp. 2342-2348, December 2004. (a) Vin PWMI PWM2 ,60ns 4OQns/div (b) Figure 11. Experimental transient response of the pulse-width modulator (a) applying step down voltage at input (b) applying step up voltage at input. 360 REFERENCES