[IEEE 2013 IEEE 20th International Conference on Electronics, Circuits, and Systems (ICECS) - Abu...
Transcript of [IEEE 2013 IEEE 20th International Conference on Electronics, Circuits, and Systems (ICECS) - Abu...
A Wideband Unity-Gain Buffer in 0.13-μm CMOSKamyar Keikhosravy, Pouya Kamalinejad, Shahriar Mirabbasi, and Victor Leung
Department of Electrical and Computer Engineering, University of British Columbia, Vancouver, BC
E-mail:{keikhosr, pkamali, shahriar, vleung}@ece.ubc.ca
Abstract—In this paper, an ultra wideband analog voltage-mode buffer is presented which can drive a load impedance of50 Ω. The presented feedback-based buffer uses a compoundamplifier which is a parallel combination of a high-DC gainoperational amplifier and a operation transconductance amplifierto achieve a high unity gain bandwidth. A proof-of-conceptprototype is designed and fabricated in a 0.13 μm CMOS process.The simulation and measurement results of the proposed bufferare in good agreement. The prototype buffer circuit consumes7.34 mW from a 1.3-V supply, while buffering a 2 GHz sinusoidalinput signal with a 0.4 V peak-to-peak (Vpp) amplitude anddriving an AC-coupled 50-Ω load.
Index Terms—Analog buffer, voltage follower, wideband buffer,CMOS.
I. INTRODUCTION
Wide-bandwidth unity-gain analog buffers are used in a
variety of high-speed and agile applications such as analog-to-
digital converters [1], switch capacitors [2], sample-and-hold
circuits[3] and active probes in measurement instruments. A
simple and commonly used architecture for such buffers is a
source-follower-based buffer[3], [2], [4]. However, achieving
high linearity and spurious-free dynamic range (SFDR) as
well as an accurate gain in such buffers are challenging
[4], although different techniques to address these problems
have been investigated[5]. In cases where the gain accuracy
and flatness are not crucial, source-follower architectures are
used for driving low impedance values such as a 50 Ωload (or a large capacitive load). In these cases, a relatively
large driving transistor is required. This large transistor in
effect limits the input bandwidth of the circuit. One way to
ameliorate this issue is to cascade multiple source-follower
stages and gradually increase the size of the transistors.
Each additional stage adds extra pole to the system which
results in deteriorating the stability and overall bandwidth
of the system. Furthermore, testing high-frequency circuits
typically requires a buffer since many high-speed integrated
circuits are not capable of driving the standard 50-Ω input
impedance of the high-frequency measurement instruments.
Thus, having a monolithic unity-gain buffer (voltage follower)
with relatively flat and accurate gain is desirable. To achieve
such a monolithic analog buffer feedback-based buffers are
typically used, e.g, using an operational amplifier in a unity-
gain feedback structure ensures a relatively accurate gain in the
presence of process, supply voltage, and temperature (PVT)
variations. Fig. 1 shows one possible architecture for such
designs. The bandwidth of this buffer is mainly limited by
the bandwidth of the operational amplifier and the size of the
driving transistor.
+
VDD_Buffer
V_Bias
AIn
Out
MD
Fig. 1. The architecture of a conventional amplifier based analog buffer.
M2 M1
M3M4
M5
Fig. 2. Architecture of compound amplifier used in this design.
In this work, we present an ultra-wideband buffer that
uses a compound amplifier similar to that presented in [6].
The presented buffer can drive 50-Ω loads while achieving a
wide bandwidth. The organization of the paper is as follows:
Section II presents the proposed architecture and provides
analytical insights. Section III presents simulation and mea-
surement results and finally Section IV concludes the paper.
II. PROPOSED ARCHITECTURE
To have an accurate flat gain, the open-loop gain of the
buffer has to be relatively large. The overall open-loop gain
of the buffer can be written as follows:
A(ω) · β(ω) = G(ω)× gm0(ω)× Zout(ω)× 1 (1)
978-1-4799-2452-3/13/$31.00 ©2013 IEEE 9
Vbias_OTA
Out
Out
In
In
OutVbias_OTA
Out
Fig. 3. The overall schematic of analog buffer presented in this work.
where G(ω) is the voltage gain of the amplifier A and gm0(ω)is the small-signal transconductance of the driving transistor
(MD in Fig. 1) at the input frequency of ω, Zout(ω) is output
impedance seen at the output node of the buffer, and β(ω) is
the feedback gain which for the structure shown in Fig. 1 is
equal to 1. The closed-loop voltage gain of the buffer can be
written as:
Vout
Vin(ω) =
A(ω)
1 +A(ω) · β(ω) =A(ω)
1 +A(ω)(2)
From (2), the overall gain of buffer in approximately 1 over the
range of frequencies where A(ω) � 1. Since for the most part
the open-loop gain of the buffer is provided by the amplifier
A, a wide bandwidth amplifier is needed. However, designing
amplifiers with both high voltage gain and high bandwidth is
challenging. One elaborate solution is the compound amplifier
introduced in [6]. The architecture of this amplifier is shown
in Fig. 2.
As shown in the figure to achieve high gain at low frequen-
cies, a high DC gain but low bandwidth amplifier, namely
an operational amplifier (opamp), is used. The operational
amplifier is in parallel with a high bandwidth operational
transconductance amplifier (OTA). The generic magnitude
frequency response of the overall buffer along with its typical
pole−zero locations is shown in Fig. 4. As described in [6],
the combination of the OTA and opamp will introduce a zero,
namely zOTA , which helps to compensate for the adverse
effects of the dominant pole of the opamp. Although the buffer
is generally connected to a small load impedance (e.g., 50 Ω),
to ensure the stability of this architecture a zero (zESR) is also
added (using a series combination of a resistor and a capacitor,
i.e., combination of RESR and Cz in Fig. 3) to the output of
the amplifier to compensate for the output load.
A. Circuit Implementation
The schematic of the presented buffer is shown in Fig. 3.
To achieve a large low-frequency gain a telescopic cascode
architecture is used for the opamp. The buffer has an input
impedance of ~8 GΩ in parallel with 127 fF (averaged from
DC to 1 GHz). For the purpose of driving a low-impedance
p
z
pzESR
p
Fig. 4. Pole-zero location of the proposed buffer
load, a relatively large driving transistor, namely, MD, is used.
The simulated frequency response of the opamp as well as that
of the OTA are shown in Fig. 5. Fig. 6 shows the frequency
response of the overall compound amplifier. The drop in the
low-frequency gain of the compound amplifier (as compared
to the opamp low-frequency gain) is due to the loading effect
of the diode-connected active load of the OTA. This gain drop
also results in pushing the dominant pole of the opamp to
higher frequencies (as can be seen in Figs. 5 and 6).
Since the buffer is expected to operate for input signals with
relatively large voltage swing, and the output of the buffer
follows the input signal, special attention should be paid to
biasing of the circuit. To put this in perspective, consider the
case that the input is a step with a large amplitude. Since
the output follows the input, both input terminals of the OTA
will experience large voltage levels which results in lowering
the drain voltage of transistors M24 and M25 of the OTA.
In this case, transistors M24 and M25 may enter the triode
region of operation. A similar scenario applies when the input
signal is at a low voltage level, where the voltage level of the
drain terminal of M26 and M27 of the OTA will increase
and therefore these pmos transistors may enter into triode
region of operation. To maintain a reasonable voltage level
at the drain of these transistors a common-mode feedback
circuitry shown in Fig. 3 consisting of an analog inverter (i.e.,
transistors M6 to M9) along with biasing circiut is used. This
feedback circuit facilitates the operation of the circuit over a
wider input voltage range by properly adjusting the tail current
10
100
102
104
106
108
1010
0
20
40
60
80
frequency (Hz)
Gai
n (d
B)
100
102
104
106
108
10100
50
100
150
200
frequency (Hz)
Pha
se m
argi
n (d
egre
e)
OTAOpamp
5.9 GHz
10.47 MHz
72°
50°
Fig. 5. Frequency response of the opamp and OTA.
100
102
104
106
108
1010
0
20
40
frequency (Hz)
Gai
n (d
B)
100
102
104
106
108
10100
50
100
150
200
frequency (Hz)
Pha
se m
argi
n (d
egre
e)
Zero Introduced by OTA3.5 GHz
45°
Fig. 6. Frequency response of the compound amplifier.
of the OTA. Fig. 7 shows the simulated output voltage of the
OTA with and without the common-mode feedback circuit.
III. EXPERIMENTAL RESULTS
A proof-of-concept prototype of the proposed buffer is
designed and fabricated in a 0.13-μm CMOS process. Fig. 9
shows the chip micrograph along with the layout view of the
buffer (the inset in the figure). The overall circuit occupies
6059 μm2. The the chip consumes 7.34 mW from a 1.3 V
supply voltage while buffering a 2 GHz sinusoidal input signal
and driving an AC-coupled 50-Ω load.
Fig. 8 shows the measured transient step response of the
buffer a small and a relatively large input steps. The simu-
lation results show that the buffer provides almost the same
performance for both small and large input steps which can
be attributed to the common-mode feedback circuit used in
the OTA. In the transient measurements (Fig. 8) the load
including the input impedance of the measurement equipment
(Tektronix DPO4054 Oscilloscope) is a 20 pF capacitive load
in parallel with a 50Ω resistor. The pulse generator used in
0 0.2 0.4 0.6 0.8 10.2
0.4
0.6
0.8
1
Input common voltage level (V)
Out
put D
C v
olta
ge o
f OT
A (
V)
With common−mode feedbackWithout common−mode feedback
Fig. 7. Simulated output voltage level of the OTA with and without thecommon-mode feedback circuit.
(a)
(b)
Fig. 8. Measured step response of the proposed buffer for (a) 350 mV and(b) 700 mV of input step amplitudes.
Fig. 9. Micrograph of the presented buffer.
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TABLE IPERFORMANCE SUMMARY AND COMPARISON WITH THE STATE-OF-THE-ART ANALOG BUFFERS.
Year Process (μm) Supply (V) Power (mW) Bandwidth (MHz) Slew rate (V/μs) Load Area (μm2)This work 2013 0.13 1.3 7.34 2000 SR− : −185, SR+:254 50 Ω || 20 pF 6059
[7] 2011 0.35 ±0.75 0.153 1.366 − 10 pF 55000[2]* 2011 0.5 1.5 0.0585 10 − 2 pF −[8] 2010 0.5 3.3 0.198 13.4 SR−:−35, SR+ :29 30 pF 17000[9] 2009 0.35 3.3 4.8 90 200 13 pF 29100
* Simulation results.
Fig. 10. Measured magnitude frequency response of the proposed buffer.
these measurements is HP8110A which can generate pulses
with a rise time of 8 ns.
The frequency response of the buffer is measured in the
closed-loop configuration. For an input signal of 400 mVpp, the
frequency response of the closed-loop buffer is measure with
an Agilent vector network analyzer E5061B and is shown in
Fig. 10. As can be seen from the figure, the 3−dB bandwidth
of the buffer is 2 GHz. The total harmonic distortion (THD)
of the buffer is measured using an Anritsu MS2034A for
a ~100 MHz input signal with a peak-to-peak amplitude of
133 mVpp . The measured result is shown in Fig. 11. The
buffer achieves a THD of ~25.5 dB. For a input signal of
1 MHz with a peak-to-peak amplitude of 270 mVppthe THD
of the buffer is −34 dB.
IV. CONCLUSION
An ultra-wide bandwidth analog buffer that uses a com-
pound amplifier in unity-gain configuration is presented. The
experimental results confirm the wideband performance of
the buffer. The bandwidth of this buffer is measured to be
2.0 GHz while it consumes 7.34 mW from a 1.3-V supply.
This design is fully monolithic and can be used in variety of
applications, in particular, for testing high-frequency circuits.
The performance summary and comparison with the state-of-
the-art designs are presented in Table. I.
V. ACKNOWLEDGMENT
This research is funded in part by the Natural Sciences
and Engineering Research Council of Canada (NSERC), a
Fig. 11. Output spectrum for a 133.33 mVpp ~100 MHz input sinusoid.
Collaborative Health Research Project (CHRP) grant, and the
Institute for Computing, Information and Cognitive Systems
(ICICS) at UBC. CAD tool support and access to technology
is facilitated by CMC Microsystems.
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