858 IEEE TRANSACTIONS ON ELECTRON DEVICES, VOL. 55, NO. 3, MARCH 2008
Threshold Voltage Variation in SOI
Schottky-Barrier MOSFETs
Min Zhang, Joachim Knoch, Shi-Li Zhang, Sebastian Feste, Michael Schr ¨ oter, Member, IEEE,
and Siegfried Mantl, Member, IEEE
Abstract—The inhomogeneity of Schottky-barrier (SB) height
Φ
B
is found to strongly affect the threshold voltage V
th
of
SB-MOSFETs fabricated in ultrathin body silicon-on-insulator
(SOI). The magnitude of this influence is dependent on gate ox-
ide thickness t
ox
and SOI body thickness t
si
; the contribution of
inhomogeneity to the V
th
variation becomes less pronounced with
smaller t
ox
and/or larger t
si
. Moreover, an enhanced V
th
variation
is observed for devices with dopant segregation used for reduction
of the effective Φ
B
. Furthermore, a multigate structure is found
to help suppress the V
th
variation by improving carrier injection
through reduction of its sensitivity to the Φ
B
inhomogeneity. A
new method for extraction of Φ
B
from room temperature transfer
characteristics is also presented.
Index Terms—Ambioplar, Schottky barrier inhomogene-
ity, Schottky barrier MOSFET, silicon-on-insulator, threshold
voltage.
I. INTRODUCTION
A
S THE CONTINUED down-scaling becomes increas-
ingly challenging, solutions are urgently needed to meet
the requirements of the International Technology Roadmap for
Semiconductors (ITRS) [1]. Schottky-barrier (SB)-MOSFETs
present a promising alternative to conventional MOSFETs,
because the metallic source–drain contacts offer abrupt
junction and low extrinsic parasitics [2], [3]. However, the
performance of SB-MOSFET still falls behind that of con-
ventional MOSFET. Therefore, intensive research has been
devoted to improving the performance of SB-MOSFETs.
Recently, a number of approaches that lead to significant
improvements of SB-MOSFETs have been demonstrated. They
include the use of silicides with lower Φ
B
(Φ
Bn
and Φ
Bp
)
Manuscript received July 6, 2007; revised October 16, 2007. The review of
this paper was arranged by Editor C.-Y. Lu.
M. Zhang was with the Institute of Bio- and Nanosystem-IBN1,
Forschungszentrum J¨ ulich, D-52454 J¨ ulich, Germany. He is now with the
Cypress Semiconductor Technology Corporation, Ltd., 201203 Shanghai,
China.
J. Knoch is with the IBM Research GmbH, Zurich Research Laboratory, 8803
R¨ uschilkon, Switzerland.
S.-L. Zhang is with the State Key Laboratory of Application Specific In-
tegrated Circuit (ASIC) and System, School of Microelectronics, Fudan Uni-
versity, 200433 Shanghai, China, and also with the School of Information and
Communication Technology, Royal Institute of Technology (KTH), SE-164 40
Stockholm, Sweden (e-mail: shilizhang@fudan.edu.cn).
S. Feste is with the Institute of Bio- and Nanosystem-IBN1, Forschungszen-
trum J¨ ulich, D-52454 J ¨ ulich, Germany.
M. Schr¨ oter is with Dresden University of Technology, 01062 Dresden,
Germany, and also with the University of California, San Diego, CA 92093
USA.
S. Mantl is with the Institute of Bio- and Nanosystem-IBN1, Forschungszen-
trum J¨ ulich, D-52454 J ¨ ulich, Germany, and also with the Aachen University of
Technology (RWTH), 52062 Aachen, Germany.
Digital Object Identifier 10.1109/TED.2007.915054
[4], [5], thin t
ox
, thin t
si
[6], or dopant segregation at the silicide–
silicon interface [7], [8]. Since a tunneling barrier is involved that
gives rise to an exponential dependence on Φ
Bn
(or Φ
Bp
) of the
injection of carriers (into the channel), the performance variation
from device to device is a major concern for SB-MOSFETs. In
particular, as SB-MOSFETs with dopant segregation are of par-
ticular interest for next generations of CMOS technology [10],
investigation of the reproducibility of such devices is becoming
urgent. In this paper, the V
th
variation in devices with different
geometric parameters as well as devices with dopant segregation
will be investigated. An analysis of the distribution of V
th
shows
that the V
th
variation induced by the Φ
B
inhomogeneity can be
effectively suppressed by the use of thin t
ox
. The use of thin t
si
,
on the other hand, leads to a larger spread in V
th
despite perfor-
mance improvement. For devices with dopant segregation, the
V
th
variation becomes slightly larger compared to the devices
without dopant segregation. The statistical mean value of V
th
is
used to extract the mean Φ
B
based on an analytical model. This
approach is different from traditionally used current vs. voltage
and temperature (I –V –T ) [9], [11], or capacitance–voltage
(C–V ) [12] methods. The extracted mean Φ
Bn
for electron
injection is 0.63 eV for devices with t
ox
= 3.5 nm and t
si
=
∼9 nm, 0.68 eV for devices with t
ox
= 3.5 nm and t
si
= ∼50 nm.
Both Φ
Bn
values satisfactorily agree with the well-documented
value determined by means of Schottky diodes [13]. Finally,
it is experimentally demonstrated that a 15% reduction of
the V
th
variation can be achieved by applying a back gate
bias.
II. SOI SB-MOSFET F ABRICATION
SB-MOSFETs with fully nickel silicided source/drain elec-
trodes were fabricated on <100> p-type doped SOI wafer
(N
A
= 1 × 10
15
cm
−3
) with an initial silicon thickness of
∼100 nm. Three series of devices were prepared: 1) t
si
=
∼50 nm, but various t
ox
; 2) t
ox
= 3.5 nm, but various t
si
; and
3) t
ox
= 3.5 nm, t
si
= ∼50 nm with dopant segregation. Devices
with different t
si
were realized by a cycle of dry/wet oxidation
and modified standard cleaning (1:8:64 = NH
4
OH:H
2
O
2
:H
2
O
at 65
◦
C for 10 min). Devices with different gate oxide thick-
nesses of 3.5 and 24 nm were realized by wet oxidation [14].
Immediately after the gate oxide formation, a 200 nm in situ
n-doped poly-Si (N
D
> 1 × 10
20
cm
−3
) and 50-nm-thick SiO
2
were deposited by means of low-pressure chemical vapor de-
position (LPCVD). The LPCVD layers were subsequently pat-
terned by reactive ion etching. Ion implantation with different
doses was only carried out for the devices with dopant segre-
gation. After sidewall spacer formation and a diluted HF dip,
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