The terahertz gap, lying roughly between 300GHz(0.3THz) and 30THz in the electromagnetic spectrum, exists because the frequencies generated by semiconductor devices based on transistors and lasers do not overlap. Generation of coherent terahertz radiation has traditionally involved either extending electronic techniques to higher frequencies or extending photonic sources to longer wavelengths. In both cases, the efficiency drops rapidly as the frequency approaches the terahertz region. We recently fabricated GaAsAlGaAs quantum cascade lasers, in which a high-confinement metal-metal waveguide was employed and fabricated using InAu metallic bonding technique. The devices demonstrated lasing operation at a wavelength of around 104.6μm (or about 2.9THz in frequency). In this article, we first present the fabrication and electrical and optical characterizations of the terahertz quantum cascade lasers. We then characterized a set of terahertz quantum cascade lasers with otherwise identical device parameters but the doping concentration. The δ-doping density for each period was varied from 3.2×1010 to 4.8×1010cm2. We observed that both the lasing threshold and the free carrier absorption caused the waveguide loss increase monotonically. Interestingly, however, the observed maximum lasing temperature displayed an optimum at a doping concentration of 3.6×1010cm2.

1.
THz Sensing and Imaging Technology
,
Springer Series in OpticalSciences
, edited by
D.
Mittleman
(
Springer
, New York,
2002
).
2.
R.
Köhler
 et al,
Nature (London)
417
,
156
(
2002
).
3.
M.
Rochat
,
L.
Ajili
,
H.
Willenberg
,
J.
Faist
,
H.
Beere
,
G.
Davies
,
E.
Linfield
, and
D.
Ritchie
,
Appl. Phys. Lett.
81
,
1381
(
2002
).
4.
B. S.
Williams
,
S.
Kumar
,
H.
Callebaut
,
Q.
Hu
, and
J. L.
Reno
,
Appl. Phys. Lett.
83
,
5142
(
2003
).
5.
B. S.
Williams
,
S.
Kumar
,
H.
Callebaut
,
Q.
Hu
, and
J. L.
Reno
,
Appl. Phys. Lett.
83
,
2124
(
2003
).
6.
R.
Köhler
 et al,
Appl. Phys. Lett.
82
,
1518
(
2003
).
7.
S.
Kumar
,
B. S.
Williams
,
S.
Kohen
,
Q.
Hu
, and
J. L.
Reno
,
Appl. Phys. Lett.
84
,
2494
(
2004
).
8.
S.
Barbieri
,
J.
Alton
,
H. E.
Beere
,
J.
Fowler
,
E. H.
Linfield
, and
D. A.
Ritchie
,
Appl. Phys. Lett.
85
,
1674
(
2004
).
9.
G.
Scalari
,
L.
Ajili
,
J.
Faist
,
H.
Beere
,
E.
Linfield
,
D.
Ritchie
, and
G.
Davies
,
Appl. Phys. Lett.
82
,
3165
(
2003
).
10.
B. S.
Williams
,
S.
Kumar
,
Q.
Hu
, and
J. L.
Reno
,
Electron. Lett.
40
,
431
(
2004
).
11.
G.
Scalari
,
S.
Blaser
,
L.
Ajili
,
J.
Faist
,
H.
Beere
,
E.
Linfield
,
D.
Ritchie
, and
G.
Davies
,
Appl. Phys. Lett.
83
,
3453
(
2003
).
12.
L.
Mahler
,
R.
Köhler
,
A.
Tredicucci
,
F.
Beltram
,
H. E.
Beere
,
E. H.
Linfield
,
D. A.
Ritchie
, and
A. G.
Davies
,
Appl. Phys. Lett.
84
,
5446
(
2004
).
13.
V. D.
Jovanovic
,
D.
Indjin
,
Z.
Ikonic
, and
P.
Harrison
,
Appl. Phys. Lett.
84
,
2995
(
2004
).
14.
B. S.
Williams
,
S.
Kumar
,
Q.
Hu
, and
J. L.
Reno
,
Opt. Express
13
,
3331
(
2005
).
15.
H.
Callebaut
,
S.
Kumar
,
B. S.
Williams
,
Q.
Hu
, and
J. L.
Reno
,
Appl. Phys. Lett.
83
,
207
(
2003
).
16.
M.
Rochat
,
M.
Beck
,
J.
Faist
, and
U.
Oesterle
,
Appl. Phys. Lett.
78
,
1967
(
2001
).
17.
D.
Indjin
,
P.
Harrison
,
R. W.
Kelsall
, and
Z.
Ikonic
,
Appl. Phys. Lett.
82
,
1347
(
2003
).
18.
Z. R.
Wasilewski
,
G. C.
Aers
,
A. J.
SpringThope
, and
C. J.
Miner
,
J. Vac. Sci. Technol. B
9
,
120
(
1991
).
19.
M.
Giehler
,
R.
Hey
,
H.
Kostial
,
S.
Cronenberg
,
T.
Ohtsuka
,
L.
Schrottke
, and
H. T.
Grahn
,
Appl. Phys. Lett.
82
,
671
(
2003
).
20.
S.
Kohen
,
B. S.
Williams
, and
Q.
Hu
,
J. Appl. Phys.
97
,
053106
(
2005
).
21.
B. S.
Williams
, Ph.D. dissertation,
Massachusetts Institute of Technology
, Cambridge, Massachusetts,
2003
.
22.
H.
Callebaut
,
S.
Kumar
,
B. S.
Williams
,
Q.
Hu
, and
J. L.
Reno
,
Appl. Phys. Lett.
84
,
645
(
2004
).
23.
D.
Indjin
,
P.
Harrison
,
R. W.
Kelsall
, and
Z.
Ikonić
,
IEEE Photonics Technol. Lett.
15
,
15
(
2003
).
24.
R. C.
Iotti
and
F.
Rossi
,
Phys. Rev. Lett.
87
,
146603
(
2001
).
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