902 IEEE TRANSACTIONS ON TERAHERTZ SCIENCE AND TECHNOLOGY, VOL. 5, NO. 6, NOVEMBER 2015
Antenna-Coupled MOSFET Bolometers for Uncooled
THz Sensing
Dan Corcos, Noam Kaminski, Evgeny Shumaker, Ofer Markish, Danny Elad, Thomas Morf, Senior Member, IEEE,
Ute Drechsler, Winnie Tatiana Silatsa Saha, Lukas Kull, Member, IEEE, Ken Wood, Ullrich R.
Pfeiffer, Senior Member, IEEE, and Janusz Grzyb
Abstract—In this paper, we present a comprehensive study on
the operation of an antenna-coupled THz bolometer based on
a micro-machined SOI-CMOS thermal sensor. The pixels are
designed to operate at room temperature in vacuum. We focus on
a new planar skirt antenna, which combines high sensitivity within
a 0.6–1.2 THz band and 30 HPBW. We present an overview of the
design considerations, as well as the characterization results which
were obtained with both broadband and CW THz sources. The
NEP of the pixel is of the order of 25 pW/Hz , with responsivity
100 mA/W at the optimal operating point. The peak responsivity
to a broadband THz signal is 600 mA/W. The ease of integration
with a read-out circuit and the low power dissipation make this
type of pixel a good candidate for focal plane array architecture.
Index Terms—Antenna-coupled bolometers, micromachined
sensors, silicon-on-insulator, terahertz (THz) imaging, uncooled
sensors.
I. INTRODUCTION
D
RIVEN by a multitude of attractive practical applica-
tions, ranging from security to medical diagnostics, from
the food industry to material inspection and astronomy, THz
imaging is a fast developing research area [1]. The challenges
involved with pushing electronic detection up to the THz
frequency range are tackled today by adopting a number of
complementary approaches. Cryogenic cooled detectors such
as transition-edge superconductor (TES) bolometers [2], [3]
and kinetic inductance detectors (KIDs) [4], [5] have demon-
strated very high sensitivity. The large footprint and large
power consumption of these detectors, as well as the reduced
pixel count may, however, limit their exploitation potential
to high-end systems only. The interest in commercial THz
applications was a main driver in recent years to efforts aimed
Manuscript received February 20, 2015; revised June 23, 2015; accepted
July 29, 2015. Date of publication August 31, 2015; date of current version
November 23, 2015. This work was supported in part by the European Union
Seventh Framework Program (FP7/2007-2013) under Grant Agreement
288442.
D. Corcos, N. Kaminski, E. Shumaker, O. Markish, and D. Elad are with
IBM Research—Haifa, Haifa University Campus, 3498825, Israel (e-mail:
dannye@il.ibm.com).
T. Morf, U. Drechsler, W. T. Silatsa Saha, and L. Kull are with IBM
Research—Zurich, 8803 Rueschlikon, Switzerland (e-mail: tmr@zurich.ibm.
com).
U. R. Pfeiffer and J. Grzyb are with the University of Wuppertal
IHCT, Bergische Universität, D-42119, Wuppertal, Germany (e-mail: ull-
rich.pfeiffer@uni-wuppertal.de).
K. Wood is with QMC Instruments Ltd., School of Physics & Astronomy,
Cardiff University, The Parade, Cardiff, CF24 3AA, U.K. (e-mail: k.wood@ter-
ahertz.co.uk).
Color versions of one or more of the figures in this paper are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TTHZ.2015.2466470
at bridging the performance gap of THz sources and room
temperature detectors. While heterostructure backward diodes
(HBD) [6] and Schottky barrier diodes (SBD) [7] are the most
sensitive solid-state detectors, SiGe HBTs are also becoming
attractive owing to the recent advancements in process and
circuit technology. The operating frequency of modern RFICs
seems inexorably to approach the 1 THz target. Signal recti-
fication has been demonstrated in transistor devices operating
well above their cut-off frequency, exploiting the plasma
wave or self-mixing effects. NEP values of 50 pW/Hz
and 14 pW/Hz have been reported for HBT-based [8] and
MOSFET-based [9] detectors respectively. These results prove
the feasibility of solid-state uncooled detector arrays with
silicon devices. Furthermore, thermal types of detectors such
as bolometers and thermopiles [10], already used in mature
infrared sensing technologies, were modified to operate below
10 THz, which is the conventional upper frequency edge of the
THz band. These solutions perform well in terms of NEP, speed
and allow high pixel counts. Micro-bolometers constructed in
vanadium oxides [11], [12] and amorphous silicon [13] have
been shown to exhibit NEP values of a few pW/Hz close
to 1 THz. These sensors lose performance at lower frequencies
due to degradation of electro-magnetic coupling efficiency.
In this work, we aim to describe the development and char-
acterization of a new MOSFET-based pixel design to act as the
building block for an uncooled THz focal plane array (FPA)
capable of passive THz imaging. Differently from previously
discussed sensors, the MOSFET bolometer relies only on the
layers already present in a standard SOI-CMOS process with
no modification. The foundry process is followed by a MEMS
bulk micro-machining process to achieve the necessary thermal
insulation. There exists a trade-off between, on one hand, better
penetration of radiation below 1 THz and, on the other hand,
higher blackbody radiation power available above 1 THz, and
we, therefore, chose our target RF band to be 0.5–1.5 THz [14].
The envisioned application is in the area of security.
II. DIRECT-COUPLING APPROACH:DESIGN CONSIDERATIONS
Since active silicon-based devices lack the capability of
signal amplification in the envisioned frequency range, we
adopted thermal sensing as the preferred approach for the de-
tection of weak THz signals. With wavelengths that are several
hundred of microns long, one main obstacle for the develop-
ment of a bolometer sensor is the design of coupling structures
(e.g., antennas or absorbers) that have adequate absorption
capability and bandwidth, without adding to thermal mass and
therefore slowing the device below a useful detection speed.
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