The ever-increasing
demand for larger bandwidth in the wired and wireless communication
markets is pushing integrated circuits to higher operation frequencies.
Traditionally, these microwave circuits have been implemented in compound
semiconductor technologies (GaAs and InP). However, silicon-based RFIC’s
have become very competitive in this arena with comparable performance,
lower cost and better system-on-a-chip (SoC) capabilities. Since silicon
suffers from larger parasitic elements both in active and passive devices,
new circuit techniques and design methodologies are needed at such high
frequencies.
Voltage-controlled
oscillators (VCO’s) are essential building blocks for frequency synthesizers
and clock-and-data recovery loops. Monolithic ring and LC oscillators
have been commonly used in such systems. Ring VCO’s have larger tuning
range and can easily generate quadrature signals, but have inferior
phase noise performance which disqualifies them in wireless and timing-critical
wired applications. LC VCO’s offer better phase noise performance, but
it becomes more difficult to achieve all the desired VCO specifications
simultaneously as the operation frequency approaches the self-resonance
frequency of on-chip inductors and the cutoff frequency of transistors.
More specifically, to operate at higher frequencies, the tank’s LC product
should decrease. However, the inductor loss, parasitic capacitances
of transistors, and loading from the output buffers do not scale at
the same rate. So L should
decrease further, which results in larger power dissipation for a given
oscillation amplitude, and more severe constraints on the tuning capability.
These limitations make it desirable to pursue alternative approaches,
such as distributed oscillators.
Distributed
oscillators originate from distributed amplifiers (a.k.a.
traveling-wave amplifiers), which have been widely used in wide-band
applications. A distributed amplifier achieves a higher gain–bandwidth
product by absorbing the parasitic capacitances of transistors into
artificial transmission lines. Correspondingly, a distributed oscillator
can potentially operate at higher frequencies than a lumped one. Also,
through a proper choice of number of stages, a distributed oscillator
can generate low-noise quadrature signals without using dividers or
poly-phase filters like in current implementations.
In order
to realize a fully-functional distributed voltage-controlled oscillator
(DVCO), new tuning techniques are needed since conventional varactor
tuning would defeat the goal of high-frequency operation and degrade
the phase noise performance. Also, a systematic and analytical approach
to the design of DVCO’s is required to be able to make accurate a priori
predictions of frequency and amplitude.
Based on
our detailed analysis, the general oscillation condition of distributed
oscillators has been derived, resulting in analytical expressions for
the frequency and amplitude. Two novel tuning techniques for DVCO’s
have been invented, namely, the inherent-varactor
tuning and patented delay-balanced
current-steering tuning. In the latter approach, the effective length
of transmission lines is varied by changing the signal path. CMOS and
bipolar DVCO’s have been designed and fabricated in a 0.35-μm BiCMOS
process. A 10-GHz CMOS DVCO achieved a tuning range of 12% (9.3–10.5
GHz), a phase noise of -103 dBc/Hz at 600 kHz offset, and output power
of 4.5 dBm without any buffering, drawing 14 mA of dc current from a
2.5-V power supply. A 12-GHz bipolar DVCO consuming 6 mA from a 2.5-V
power supply has also been demonstrated. It has a tuning range of 26%
with a phase noise of -99 dBc/Hz at 600 kHz offset.