1498 IEEE ELECTRON DEVICE LETTERS, VOL. 32, NO. 11, NOVEMBER 2011
Sub-10-nm Tunnel Field-Effect Transistor
With Graded Si/Ge Heterojunction
Chun-Hsing Shih and Nguyen Dang Chien
Abstract—This study presents a new sub-10-nm tunnel field-
effect transistor (TFET) with bandgap engineering using a graded
Si/Ge heterojunction. Both the height and width of the tunneling
barrier are highly controlled by applying gate voltages to ensure a
near ideal sub-5-mV/dec switching of scaled sub-10-nm TFETs at
300 K. This study performed a 2-D simulation to elucidate p-body
graded Si/Ge heterojunction TFET devices from 50 to 5 nm. The
ON-state tunneling barrier around the source was narrowed and
lowered to demonstrate a high ON-current; simultaneously, the
OFF-state tunneling barrier was raised and extended into the drain
to control the short-channel effect and ambipolar leakage cur-
rent. The shorter the length is, the more abrupt is the switching.
The breakthrough in subthreshold swing and short-channel effect
make the graded Si/Ge TFET highly promising as an ideal green
transistor into sub-10-nm regimes.
Index Terms—Bandgap engineering, graded Si/Ge heterojunc-
tion, short-channel effect, tunnel field-effect transistor (TFET).
I. I NTRODUCTION
T
UNNEL field-effect transistor (TFET) has demonstrated
the potential to surpass the subthreshold swing limit of
60 mV/dec at 300 K, both theoretically and experimentally
[1]–[3], and serves as an attractive candidate for low-power
applications [1], [4]. A minimized subthreshold swing with a
high ON-current and low OFF-current is the key requirement
for a TFET to be an ideal switching device. A silicon-based
TFET exhibits a low OFF-current and minimized subthreshold
swing; however, it suffers from a low ON-current because of
its relatively high energy bandgap [1], [3], [5]. Small-bandgap
semiconductors, such as SiGe and Ge, have been introduced
in TFET devices for boosting the ON-current. Unfortunately,
ambipolar OFF-current is increased correspondingly [5], [6].
Several gate engineering methods using high-k gate
dielectrics have been utilized to enhance the ON-current and
suppress the OFF-current [7]–[9]. Alternatively, channel engi-
neering techniques using asymmetric silicon–germanium sub-
strates have been employed to generate favorable switching
characteristics [4], [10]–[13]. Although those approaches have
promoted the merits of long-channel TFET devices, scaling
TFET length (L
g
) into sub-20-nm regimes is still a consider-
able challenge [14]. Introducing high-k dielectrics and double-
gate structure offers a stronger gate control to salvage TFETs
Manuscript received July 12, 2011; revised July 29, 2011; accepted
August 2, 2011. Date of publication September 25, 2011; date of current version
October 26, 2011. The review of this letter was arranged by Editor X. Zhou.
The authors are with the Department of Electrical Engineering, National Chi
Nan University, Nantou 54561, Taiwan (e-mail: shihch@ncnu.edu.tw).
Color versions of one or more of the figures in this letter are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/LED.2011.2164512
partly from short-channel effect [14], [15]. However, short-
channel effect is extremely pronounced into sub-20-nm regimes
due to the presence of direct drain-to-source tunneling [9] and
the penetration of lateral electrical field [14]. Using small-
bandgap semiconductors widens active tunneling regions, con-
straining the device scaling further.
To scale TFETs into sub-10-nm regimes, this study proposes
a new graded Si/Ge heterojunction to tailor the on–off switch-
ing tunneling barrier. Using this architecture, both the height
and width of the tunneling barrier are controlled precisely
using gate voltages to ensure an ideal device switching. A 2-D
simulation [16] was performed to study a p-body TFET us-
ing a graded Si/Ge heterojunction. Section II describes the
device structures and simulation parameters of TFET devices.
Section III discusses the mechanism of bandgap engineering
and presents the device characteristics of the ON-/OFF-current
and subthreshold swing in sub-10-nm TFET devices.
II. DEVICE STRUCTURES AND SIMULATION PARAMETERS
Fig. 1(a) shows the schematic sketch of a p-body TFET with
a graded Si/Ge heterojunction, where counterpart uniform Ge
and abrupt heterojunction TFETs are also shown for compar-
ison. A double-gate structure and 10-nm body thickness were
used with a 4.8-eV gate work function and 3-nm HfO
2
gate
dielectric for low subthreshold swing and high current density
[4], [15]. A heavily doped n+ source of 10
20
cm
−3
and p+
doped drain of 5 × 10
18
cm
−3
were utilized with a p-body of
10
17
cm
−3
to improve the ON-current and subthreshold swing
and to reduce the ambipolar leakage current [1], [6], [11].
In numerical simulations, the graded Si/Ge heterojunction is
assumed linearly while considering physical tunneling models
[6], [16]. For the abrupt heterostructure TFET, an optimized
p-channel TFET (Si-drain, Si-channel, and Si
0.7
Ge
0.3
-source)
[13] with a gate work function of 5.27 eV was utilized to ensure
a competitive heterojunction device. The selection of a 0.3 Ge
mole fraction and 2-nm gate–source overlap was based on the
optimization of a high ON-current, low OFF-current, and steep
subthreshold swing [13].
Fig. 1(b) shows the energy-band diagrams of 50-nm graded
Si/Ge TFETs along channel surface in on and off states. Under
the ON-state condition, the graded Si/Ge TFET has a narrow
tunneling barrier to generate a high ON-current. In the OFF state,
the tunneling barrier is considerably large to control the leakage
current. Notably, a gradually wide and high barrier is observed
from the source to the drain in the graded Si/Ge TFET, which
is different from that in a uniform Ge TFET. This feature of the
tunneling barrier plays a key role in suppressing short-channel
effect and OFF-state current in scaled TFETs.
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