Terahertz (THz) electromagnetic spectrum draws wide attention for nondestructive and/or biocompatible sensing. In order to be widely applicable to the THz sensing, it is of prime importance to develop THz sensors that can be operated at room temperature and have high sensitivity and fast operation speed. However, conventional room-temperature THz thermal sensors fall short of expectations in these characteristics required in various applications of THz sensing, including THz cameras. Utilizing a thermomechanical transduction scheme, we have developed an uncooled, sensitive, and fast THz bolometer by using a doubly clamped GaAs microelectromechanical system (MEMS) beam resonator as a sensitive thermistor. Owing to its ultrahigh temperature sensitivity (the noise equivalent temperature difference of ∼1 μK/√Hz), the present bolometer achieves not only high sensitivity but also an operation bandwidth of several kHz, which is more than 100 times faster than other uncooled THz thermal sensors. The obtained electrical noise equivalent power is as low as ∼90 pW/√Hz, which is close to the limit set by the thermal fluctuation noise. The MEMS bolometers are fabricated by the standard semiconductor fabrication processes and are well suited for making detector arrays for realizing THz cameras.

1.
M.
Tonouchi
,
Nat. Photon.
1
,
97
(
2007
).
2.
R. C.
Jones
,
J. Opt. Soc. Am.
43
,
1
(
1953
).
3.
P. L.
Richards
,
J. Appl. Phys.
76
,
1
(
1994
).
4.
D. H.
Andrews
,
R. M.
Milton
, and
W.
DeSorbo
,
J. Opt. Soc. Am.
36
,
518
(
1946
).
5.
K.
Ekinci
and
M.
Roukes
,
Rev. Sci. Instrum.
76
,
061101
(
2005
).
6.
A.
Boisen
,
S.
Dohn
,
S. S.
Keller
,
S.
Schmid
, and
M.
Tenje
,
Rep. Prog. Phys.
74
,
036101
(
2011
).
7.
A. N.
Cleland
,
Foundations of Nanomechanics: From Solid-State Theory to Device Applications
(
Springer Science & Business Media
,
2013
).
8.
K. L.
Ekinci
,
X. M. H.
Huang
, and
M. L.
Roukes
,
Appl. Phys. Lett.
84
,
4469
(
2004
).
9.
K.
Jensen
,
K.
Kim
, and
A.
Zettl
,
Nat. Nanotech.
3
,
533
(
2008
).
10.
A. N.
Cleland
and
M. L.
Roukes
,
Nature
392
,
160
(
1998
).
11.
S. C.
Masmanidis
,
H. X.
Tang
,
E. B.
Myers
,
M.
Li
,
K.
De Greve
,
G.
Vermeulen
,
W.
Van Roy
, and
M. L.
Roukes
,
Phys. Rev. Lett.
95
,
187206
(
2005
).
12.
K.
Onomitsu
,
I.
Mahboob
,
H.
Okamoto
,
Y.
Krockenberger
, and
H.
Yamaguchi
,
Phys. Rev. B
87
,
060410
(
2013
).
13.
A. K.
Pandey
,
O.
Gottlieb
,
O.
Shtempluck
, and
E.
Buks
,
Appl. Phys. Lett.
96
,
203105
(
2010
).
14.
X. C.
Zhang
,
E. B.
Myers
,
J. E.
Sader
, and
M. L.
Roukes
,
Nano Lett.
13
,
1528
(
2013
).
15.
Y.
Hui
and
M.
Rinaldi
,
Appl. Phys. Lett.
102
,
093501
(
2013
).
16.
Y.
Zhang
,
Y.
Watanabe
,
S.
Hosono
,
N.
Nagai
, and
K.
Hirakawa
,
Appl. Phys. Lett.
108
,
163503
(
2016
).
17.
Y.
Zhang
,
S.
Hosono
,
N.
Nagai
, and
K.
Hirakawa
,
Appl. Phys. Lett.
111
,
023504
(
2017
).
18.
J. C.
Mather
,
Appl. Opt.
21
,
1125
(
1982
).
19.
F. J.
Low
,
J. Opt. Soc. Am.
51
,
1300
(
1961
).
20.
I.
Mahboob
and
H.
Yamaguchi
,
Nat. Nanotech.
3
,
275
(
2008
).
21.
T. R.
Albrecht
,
P.
Grütter
,
D.
Horne
, and
D.
Rugar
,
J. Appl. Phys.
69
,
668
(
1991
).
22.
A. A.
Andronov
,
A. A.
Vitt
, and
S. E.
Khaikin
,
Theory of Oscillators: Adiwes International Series in Physics
(
Elsevier
,
2013
).
23.
The PLL model used in this work was Nanonis Oscillation Controller (OC4), from SPECS Zurich GmbH.
24.
S.
Liu
and
D.
Long
,
Proc. IEEE
66
,
14
(
1978
).
25.
P.
Muralt
,
Rep. Prog. Phys.
64
,
1339
(
2001
).
26.
H.
Jerominek
,
F.
Picard
, and
D.
Vincent
,
Opt. Eng.
32
,
2092
(
1993
).
27.
B. E.
Cole
,
R. E.
Higashi
,
J. A.
Ridley
, and
R. A.
Wood
,
Proc. SPIE
4369
,
235
(
2001
).
28.
N.
Oda
,
H.
Yoneyama
,
T.
Sasaki
,
M.
Sano
,
S.
Kurashina
,
I.
Hosako
,
N.
Sekine
,
T.
Sudoh
, and
T.
Irie
,
Proc. SPIE
6940
,
69402
(
2008
).
29.
T.
Fukuma
,
M.
Kimura
,
K.
Kobayashi
,
K.
Matsushige
, and
H.
Yamada
,
Rev. Sci. Instrum.
76
,
053704
(
2005
).
30.
D.
Antonio
,
D. H.
Zanette
, and
D.
López
,
Nat. Commun.
3
,
806
(
2012
).
31.
The thermal time constant, τ, of a bolometer is given by CT/GT (CT denotes the heat capacitance of the photoactive area). Since the NETD of the present MEMS bolometer is very small (1μK/√Hz), we can use a large GT to achieve a short thermal time constant, while keeping the MEMS bolometer sensitive.
32.
The THz source used in this work was Tera-Master, from Spectra Quest Lab, Inc.
33.
T.
Nagatsuma
and
H.
Ito
,
Advances in Photodiodes
(
InTech
,
2011
).
34.
K.
Aydin
,
V. E.
Ferry
,
R. M.
Briggs
, and
H. A.
Atwater
,
Nat. Commun.
2
,
517
(
2011
).
35.
C.
Hilsum
,
J. Opt. Soc. Am.
44
,
188
(
1954
).

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