IEEE MICROWAVE AND WIRELESS COMPONENTS LETTERS, VOL. 18, NO. 3, MARCH 2008 215
A 220 GHz (G-Band) Microstrip MMIC
Single-Ended Resistive Mixer
Sten E. Gunnarsson, Student Member, IEEE, Niklas Wadefalk, Iltcho Angelov, Member, IEEE,
Herbert Zirath, Member, IEEE, Ingmar Kallfass, and Arnulf Leuther
Abstract—This letter presents the design and characterization
of a 220 GHz microstrip monolithic microwave integrated circuit
single-ended resistive mixer in a 0.1 GaAs mHEMT tech-
nology. A conversion loss as low as 8.7 dB is obtained, limited
by the available local oscillator (LO) power (1.5 dBm) in the
measurement setup. The radio frequency (RF) bandwidth is also
limited by the measurement setup, but the mixer demonstrates a
flat response over the measured 200 to 220 GHz frequency range.
Furthermore, measured intermediate frequency bandwidth, 1-dB
input compression point, LO-to-RF isolation, and reflection coef-
ficients are presented and discussed.
Index Terms—GaAs, G-band, imaging, mHEMT, microstrip,
millimeter-wave, monolithic microwave integrated circuit
(MMIC), single-ended resistive mixer, 220 GHz.
I. INTRODUCTION
M
ONOLITHIC microwave integrated circuits (MMICs)
and systems operating beyond 100 GHz have gained
increased academic and commercial interest over the recent
years. Applications include radiometers measuring the absorp-
tion lines of e.g., oxygen (118 GHz) and water (183 GHz) for
environmental studies. The atmospheric windows at 94, 140,
and 220 GHz have been proposed and used for high-resolu-
tion passive and active millimeter-wave (mm-wave) imaging
applications such as through-wall imaging and detection of
concealed weapons, plastic explosives, and biological weapons.
Clearly, such systems should ideally be small and lightweight
mobile units which easily could be moved to the place of
operation. Thus, a MMIC based solution would be favorable
over a traditional waveguide solution due to its smaller size
and weight. Furthermore, a MMIC solution with its lower price
per unit and high manufacturing repeatability opens up the
possibility of multi-pixel systems with several receivers and/or
transmitters for enhanced system performance.
Manuscript received October 1, 2007; revised November 15, 2007. This work
was supported by the Swedish Defense Agency (FOI) through the NanoComp
Project (a Swedish/German Research Collaboration together with the Swedish
Foundation for Strategic Research (SSF) through the High Speed Electronics
and Photonics (HSEP) Program), and by the Fraunhofer Institute for Applied
Solid-State Physics (IAF).
S. E. Gunnarsson, N. Wadefalk, and I. Angelov are with the Microwave Elec-
tronics Laboratory, Department of Microtechnology and Nanoscience - MC2,
Chalmers University of Technology, Göteborg SE-412 96, Sweden (e-mail: sten.
gunnarsson@chalmers.se)
H. Zirath is with the Microwave Electronics Laboratory, Department of Mi-
crotechnology and Nanoscience - MC2, Chalmers University of Technology,
Göteborg SE-412 96, Sweden and also with the Microwave and High Speed
Electronics Research Center, Ericsson AB, Mölndal SE-431 84, Sweden.
I. Kallfass and A. Leuther are with the Fraunhofer Institute for Applied Solid
State Physics (IAF), Freiburg 79108, Germany.
Digital Object Identifier 10.1109/LMWC.2008.916819
Regarding MMIC design for very high frequencies, a few
MMICs operating at H-band (220–325 GHz) have been pub-
lished and these include voltage controlled oscillators (VCOs)
[1] and low noise amplifiers (LNAs) [2]. Large-signal de-
signs such as power amplifiers (PAs), multipliers, and mixers
operate at much lower frequencies compared to VCOs and
small-signal amplifiers for a given technology. Very few
G-band (140–220 GHz) and no H-band large-signal MMIC
designs are presented in the open literature but the existing
G-band publications include for example [3] on multipliers.
Mixers are equally rare, with only one mixer characterized up
to 210 GHz, [4].
Thus, there is a need to explore the performance of MMIC
mixers operating at G-band and beyond. Furthermore, almost
all of the mentioned designs are made in coplanar waveguide
(CPW) technologies due to its simplified processing and better
high frequency performance due to the reduced source induc-
tance compared to microstrip line designs. However, to sim-
plify the layout and to shrink the size of complex multi-func-
tional MMICs, microstrip designs are of particular interest. This
work presents a microstrip MMIC mixer which operates up to
220 GHz. The upper frequency is limited by the measurement
setup rather than the mixer itself.
II. MIXER TOPOLOGY AND DESIGN
The mixer was manufactured in a 0.1 gate length GaAs
metamorphic high electron mobility transistor (mHEMT)
MMIC process offered by the Fraunhofer Institute for Applied
Solid-State Physics (IAF) in Germany, [5]. A 2 20
mHEMT microstrip device on the standard 50 thick GaAs
substrate from this process has and of 170 and
GHz, respectively. In circuits like resistive mixers
when the HEMT device operates as a gate-voltage controlled
resistor with zero drain bias, versus is an important
parameter. For maximum conversion efficiency in such circuits,
the HEMT would ideally switch between infinite off- and zero
on-resistance. Particularly, the on-resistance needs to be low
since the off-resistance in practical circuits is high enough for
efficient switching. The on-resistance for the mHEMT device is
0.5 . A more comprehensive description of this process
can be found in [3].
The devices are modeled and characterized within our group
at Chalmers. The Chalmers FET model (also known as the An-
gelov model) was chosen due to its suitability for large signal
designs such as power amplifiers, multipliers, and mixers. The
model predicts not only and capacitance characteristic,
but also its derivatives in a correct way without discontinuities
for positive and negative drain voltages. The device model
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