1446 IEEE TRANSACTIONS ON ELECTRON DEVICES, VOL. 54, NO. 6, JUNE 2007
Scalability of Stress Induced by Contact-Etch-Stop
Layers: A Simulation Study
Geert Eneman, Peter Verheyen, An De Keersgieter, Malgorzata Jurczak, and Kristin De Meyer, Senior Member, IEEE
Abstract—This paper presents a study on the effectiveness of
strained contact-etch-stop-layer (CESL) technologies in aggres-
sively scaled dense structures. The focus is on nested transistors,
which is a technologically very important structure that consists
of a chain of gates on one active area. It will be shown that the
two main channel stress components introduced by CESL, which
are the vertical and parallel stresses, have a different sensitivity
toward layout variations, which accordingly leads to different
scaling guidelines to obtain a layout-insensitive strained CESL
technology. Decreasing the CESL thickness is not enough for
technology scaling; also, adapting the spacer dimensions is indis-
pensable to scale a strained CESL technology from one technology
node to the next.
Index Terms—MOSFET, strained-silicon.
I. INTRODUCTION
T
HE USE of mechanical strain has become a significant
booster for silicon CMOS technology over the last five
years. Strain changes the semiconductor’s band structure and
modulates the conduction mass and intervalley and interband
scattering properties of electrons and holes. This in turn
can improve or degrade the characteristics for n- and p-type
MOSFETs.
One promising technique to introduce strain inside a transis-
tor channel is the use of a silicon-nitride contact-etch-stop layer
(CESL) with an intrinsic stress [1]–[8]. This layer is deposited
in a CMOS flow after the source/drain (S/D) and gate silici-
dation module, and serves as a stopping layer for the contact
etching between the first level of metal and the transistor’s S/D
and gate regions. CESL has a typical thickness of 20 nm and can
contain up to 3 GPa of tensile or compressive stress, depending
on the deposition conditions. The intrinsic stress inside the
CESL translates into a stress state in the MOS channel. For
short-channel transistors, a CESL with tensile intrinsic stress
improves the nMOS performance, while a compressive intrinsic
stress is beneficial for the pMOS behavior [1], [3], [7], [8].
Manuscript received November 27, 2006; revised February 22, 2007. The
review of this paper was arranged by Editor V. R. Rao.
G. Eneman is with the Interuniversity Microelectronics Center (IMEC), 3001
Leuven, Belgium. He is also with the ESAT-INSYS, Katholieke Universiteit
Leuven, 3000 Leuven, Belgium, and with the Fund for Scientific Research,
1000 Brussels, Belgium.
P. Verheyen, A. De Keersgieter, and M. Jurczak are with the Interuniversity
Microelectronics Center (IMEC), 3001 Leuven, Belgium.
K. De Meyer is with the Interuniversity Microelectronics Center (IMEC),
3001 Leuven, Belgium, and also with the ESAT-INSYS, Katholieke Univer-
siteit Leuven, 3000 Leuven, Belgium.
Digital Object Identifier 10.1109/TED.2007.896367
Fig. 1. Top-view layout of (left) a nested-transistor structure and (right) the
corresponding electrical circuit.
Similar to the SiGe S/D-technology, which is used to gener-
ate a compressive channel stress in pMOS transistors, the CESL
technology is a local stress technique. Both techniques have
the advantage that the induced channel stress increases if the
transistor length is scaled. On the other hand, the channel stress
is a function of other structural dimensions as well. For CESL,
important parameters are the CESL thickness, the transistor’s
gate length and height, the intrinsic stress in the CESL, the
spacer thickness [5], [9], and the active-area length and width
[10]. These dependences complicate technology modeling and
make a thorough understanding of CESL-induced stress indis-
pensable for the design of digital and analog circuits.
The purpose of this paper is to investigate the sensitivity of
CESL-induced stress toward one specific important dimension:
the active-area size and poly-to-poly length in aggressively
scaled nested transistors. A nested-transistor structure is a chain
of gates on one active area, which is separated by a distance of
L
p/p
, which is the poly-to-poly length. This structure is a basic
building block in CMOS technology (Fig. 1). It is intuitively
clear that in scaled nested structures, the amount of CESL
between the consecutive poly lines is reduced, which may lead
to a decreased effectiveness of the technology.
The stress simulations in this paper are performed with the
finite-element simulator Taurus-Process of Synopsys [11]. The
focus is on short-channel transistors (L
g
< 50 nm), and we use
the stress in the center of the channel, 1 nm below the silicon
surface (Fig. 2), as a measure for the CESL-induced stress. The
goal is to indicate how channel stress changes as a function
of active-area length and to point out the essential differences
between the two stress components induced by CESL in the
channel, the parallel and vertical stresses. All simulated nested
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