JOURNAL OF MICROELECTROMECHANICAL SYSTEMS, VOL. 20, NO. 5, OCTOBER 2011 1201
Multistage Planar Thermoelectric Microcoolers
Andrew J. Gross, Gi Suk Hwang, Baoling Huang, Hengxi Yang, Niloufar Ghafouri, Student Member, IEEE,
Hanseup Kim, Member, IEEE, Rebecca L. Peterson, Member, IEEE, Ctirad Uher,
Massoud Kaviany, Fellow, ASME, and Khalil Najafi, Fellow, IEEE
Abstract—Many types of microsystems and microelectro-
mechanical systems (MEMS) devices exhibit improved perfor-
mance characteristics when operated below room temperature.
However, designers rarely pair such devices with integrated cool-
ing solutions because they add complexity to the system and often
have power consumption which far exceeds that of the microsys-
tem itself. We report the design, fabrication, and testing of both
one- and six-stage thermoelectric (TE) microcoolers that target
MEMS applications through optimization for low-power opera-
tion. Both coolers use thin-film Bi
2
Te
3
and Sb
2
Te
3
as the n- and
p-type TE materials, respectively, and operate in a planar configu-
ration. The six-stage cooler has demonstrated a ΔT = 22.3
◦
C at
a power consumption of 24.8 mW, while the one-stage cooler has
demonstrated a ΔT = 17.9
◦
C at a lower power consumption of
12.4 mW. [2011-0087]
Index Terms—Microcooler, microelectromechanical systems
(MEMS), solid-state cooling, thermoelectric (TE) devices.
Manuscript received March 22, 2011; revised June 8, 2011; accepted
July 7, 2011. Date of publication August 30, 2011; date of current version
September 30, 2011. This work was supported by the Micro Cryogenic
Coolers Program of the Defense Advanced Research Projects Agency under
Grant W31P4Q-06-1-001. Portions of this work were performed at the Lurie
Nanofabrication Facility, a member of the National Nanotechnology Infrastruc-
ture Network, which is supported in part by the National Science Foundation.
The work of M. Kaviany was also supported by the World Class University
program through the National Research Foundation of Korea, Ministry of
Education, under Grant R31-30005. Subject Editor C.-J. Kim.
A. J. Gross was with the Electrical Engineering and Computer Science
Department, University of Michigan, Ann Arbor, MI 48109 USA. He is now
with Sandia National Laboratories, Albuquerque, NM 87185 USA (e-mail:
ajgross@umich.edu).
G. S. Hwang was with the Mechanical Engineering Department, University
of Michigan, Ann Arbor, MI 48109 USA. He is now with the Environmen-
tal Energy Technologies Division, Lawrence Berkeley National Laboratory,
Berkeley, CA 94720 USA (e-mail: gshwang@lbl.gov).
B. Huang was with the Mechanical Engineering Department, University of
Michigan, Ann Arbor, MI 48109 USA. He is now with the Department of Me-
chanical Engineering, The Hong Kong University of Science and Technology,
Kowloon, Hong Kong (e-mail: mebhuang@ust.hk).
H. Yang and C. Uher are with the Physics Department, University
of Michigan, Ann Arbor, MI 48109 USA (e-mail: hxyang@umich.edu;
cuher@umich.edu).
N. Ghafouri, R. L. Peterson, and K. Najafi are with the Electrical Engineer-
ing and Computer Science Department, University of Michigan, Ann Arbor,
MI 48109-2122 USA (e-mail: nghafour@umich.edu; blpeters@umich.edu;
najafi@umich.edu).
H. Kim was with the Electrical Engineering and Computer Science Depart-
ment, University of Michigan, Ann Arbor, MI 48109 USA. He is now with the
Electrical and Computer Engineering Department, The University of Utah, Salt
Lake City, UT 84112 USA (e-mail: hanseup@ece.utah.edu).
M. Kaviany is with the Mechanical Engineering Department, University of
Michigan, Ann Arbor, MI 48109 USA, and also with the Division of Advanced
Nuclear Engineering, Pohang University of Science and Technology, Pohang
790-784, Korea (e-mail: kaviany@umich.edu).
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/JMEMS.2011.2163302
I. I NTRODUCTION
T
HE NEED for microscale coolers is driven by micro-
electromechanical systems (MEMS) and electronic de-
vices, such as resonators, gyroscopes, infrared sensors, and
low-noise amplifiers, which exhibit enhanced performance
when operated at temperatures below ambient. Resonant
MEMS, in particular, have very low power dissipation, and
many of the applications that integrate them seek to exploit
these low-power features as well as their small size [1]. As a
result, any cooling device designed for integration with these
low-power MEMS devices should itself be both low power and
compact.
One approach to microscale cooling has been the develop-
ment of miniaturized Joule–Thompson (J–T) coolers [2]–[6].
Some of these devices have effectively produced temperature
differentials of 192 K with heat loads up to 16 mW, using a
heat exchanger with a size of 2 mm × 35 mm × 1 mm [2].
However, the heat exchanger alone does not define a complete
J–T cooling system. J–T coolers also require a source of com-
pressed gas, which can be supplied by an external pressurized
source [3] or by an attached compressor [7]. The lack of small
simple implementation makes J–T coolers impractical for many
microcooling applications.
Thermoelectric (TE) cooling, although less efficient than J–T
cooling, relies on solid-state operating principles that can be
scaled to the microdomain. As a result, TE cooling can be
effectively utilized in applications that require small, simple,
and robust coolers. Additionally, TE materials can be deposited
and patterned at the wafer level with standard microfabrica-
tion techniques, making batch-mode production a possibility.
Microscale TE coolers have been previously demonstrated by
several groups [8]–[18] representing a wide range of choices
in cooler design, TE materials, and fabrication techniques. A
summary of devices from industry and academia is provided
in Table I. The best performing coolers in this group are
able to generate temperature differentials between 40 K and
100 K; however, they require power inputs of several hundred
milliwatts or more. Such high power consumption makes these
coolers incompatible with MEMS integration in many applica-
tions. On the other hand, the low-power coolers to date have
not demonstrated enough total temperature differential to be
useful in achieving meaningful performance gains from the
target electronics and MEMS devices. This paper presents a
TE microcooling solution that can generate reasonably large
temperature differences with very small power.
The special features of micro TE coolers, including size ef-
fects and interfacial transport phenomena, are addressed in [19].
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