IEEE JOURNAL OF SOLID-STATE CIRCUITS, VOL. 42, NO. 12, DECEMBER 2007 2715
40-Gb/s High-Gain Distributed Amplifiers With
Cascaded Gain Stages in 0.18- m CMOS
Jun-Chau Chien, Student Member, IEEE, and Liang-Hung Lu, Member, IEEE
Abstract—A novel circuit topology for high-gain distributed am-
plifiers is presented in this study. Based on the conventional dis-
tributed architecture, the gain cells are realized by cascading cas-
code stages for gain enhancement. In addition, the stagger-tuning
technique is extensively utilized in the design of the cascode stages
as well as the cascaded stages, leading to significant improvement
in terms of the operating bandwidth and the gain flatness. With the
proposed circuit architecture, two amplifiers are implemented in a
standard 0.18- m CMOS technology. The amplifier with a 3 3
configuration exhibits a gain of 16.2 dB and a 3-dB bandwidth of
33.4 GHz, while the one in a form of 2 4 demonstrates a gain
of 20 dB and a bandwidth of 39.4 GHz. Consuming a dc power
of 260 mW from a 2.8-V supply voltage, both circuits provide clear
eye-opening with a pseudorandom bit sequence (PRBS) at 40 Gb/s.
Index Terms—Bandwidth enhancement, distributed amplifiers,
gain–bandwidth product, gain flatness, inductive peaking, stagger-
tuning technique.
I. INTRODUCTION
D
UE TO THE increasing demand in the capacity of data
communications, implementation of systems operating at
a data rate beyond 10 Gb/s has attracted great attention in the
past decade. With the advances in semiconductor technologies,
integrated circuits operating at 40 Gb/s have been realized in
standard CMOS processes [1]–[5]. Among all kinds of high-
speed circuits, the broadband amplifier is a key building block
at both the transmitting and the receiving ends. Recently, sev-
eral CMOS broadband amplifiers with bandwidth-enhancement
techniques have been reported [6]–[10].
In conventional circuit implementations, the gain-bandwidth
product of broadband amplifiers is severely limited by the
process technology. For high-speed operations, the amplifier
gain is often sacrificed for an adequate bandwidth. Therefore,
most of the 40-Gb/s amplifiers suffer from a limited gain [9],
[10]. In order to overcome the design limitations, a novel circuit
architecture for broadband amplifiers is proposed in this study
[11]. By replacing the gain cells in the conventional distributed
amplifiers (DAs) with cascaded stages, the gain is effectively
enhanced. In addition, due to the use of inductive peaking with
the stagger-tuning technique, a remarkable 3-dB bandwidth can
be achieved while maintaining excellent gain flatness within
the entire frequency band.
Manuscript received April 11, 2007; revised August 27, 2007. This work was
supported in part by the National Science Council under Grants 96-2220-E-
002-016 and 96-2220-E-002-018.
The authors are with the Department of Electrical Engineering and Graduate
Institute of Electronics Engineering, National Taiwan University, Taipei 10617,
Taiwan, R.O.C. (e-mail: lhlu@cc.ee.ntu.edu.tw).
Digital Object Identifier 10.1109/JSSC.2007.908688
Fig. 1. Simplified circuit schematic of a 1-D DA.
This paper is organized as follows. Section II discusses the
existing architectures for broadband amplifiers and introduces
the proposed circuit configuration. Detailed circuit design and
experimental results of the 40-Gb/s high-gain DAs are presented
in Sections III and IV, respectively. Finally, conclusions are pro-
vided in Section V.
II. AMPLIFIER ARCHITECTURE
A. Conventional DA
Distributed circuit techniques are widely used for the broad-
band amplifiers in high-speed data links [10]–[16] as well as
the low-noise amplifiers in ultra-wideband (UWB) systems
[17]–[19]. Fig. 1 shows the simplified schematic of the conven-
tional one-dimensional (1-D) DA. Note that each gain cell is
represented by a common-source stage for simplicity. By prop-
erly choosing the transistor sizes and the inductance values, the
input and the output of the amplifier can be treated as 50-
artificial transmission lines, demonstrating extremely wideband
frequency response with low input and output return losses. In
order to maximize the gain of the amplifier, the phase delays
of the input and the output transmission lines are typically
matched. Therefore, the currents generated by the individual
gain cells can be added constructively at the output of the
amplifier. Assuming that the transmission lines are lossless, the
low-frequency gain of the 1-D DA can be estimated by
(1)
where is the number of the distributed stages, represents
the transconductance of each stage, and is the termination
impedance for the output transmission line, which is typically
50 . Note that the coefficient 1/2 in (1) indicates that half of the
signal current propagates in an opposite direction towards the
drain termination. The characteristic impedance and the phase
velocity of the artificial transmission lines can be expressed as
(2)
(3)
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