Uploaded by Dr. Saravanakumar Chandrasekaran

Need for FINFET SOI

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Finfet with isolated n+ and p+ gate regions strapped with Metal and Polysilicon
L. Mathew , M. Sadd, B. E. White, A. Vandooren, S. Dakshina-Murthy*, J. Cobb, T. Stephens, R.. Mora,
D. Pham , J. Conner, T. White, Z. Shi, A.V-Y Thean, A. Barr, M. Zavala, J. Schaeffer, M.J. Rendon,
D. Sing, M. Orlowski, B.-Y. Nguyen, J. Mogab
APRDL, DigitalDNA Laboratories 3501 Ed Bluestein Blvd.MD: K10
Motorola Inc-Semiconductor Products Sector (*Motorola-AMD alliance)
3501 Ed Bluestein blvd. Austin TX-7872, U.S.A : ( r26180@email.sps.mot.com, phone: 512 933 2385)
Abstract
A vertical double Gate MOSFET structure with a new gate
stack architecture has been demonstrated. The Gate stack
consists of two isolated polysilicon regions that are doped N+
and P+ with a metal/polysilicon strap connecting the doped
regions. The device has an undoped channel yet performs as
an enhancement mode MOSFET due to the asymmetric
doping of the gate regions on either side of the channel. The
advantages of this structure include: 1) reduction of the Vt
variations caused by dopant fluctuation in the channel region
2) enhanced mobility due to an undoped channel region 3)
flexibility to adjust Vt across a wide range from depletion
mode to very high Vt depending on the application 4) lower
interconnect resistance due to the use of metal/polysilicon
gate components 5) better manufacturability due to easier
patterning of gate over spacer. The devices are enhancement
mode with Vt ~= (0.1-0.3V) at 100nm gate length and
channel thickness of less than 30nm and height 100nm tall
have been demonstrated. Functional devices at the 100nm
gate have Ion =191 µA/ µm , Vt = 0.3V Ioff = 0.5 µA/ µm
SS=94 mV/decade.. A different device with different implant
dose and drive demonstrated Vt = 0.15V and
SS=80mV/decade at Lgate=0.25µm.
N+
Channel
Metal
Introduction
Double gate MOSFET structures have been studied to replace
the traditional planar CMOS structures [1-5]. These devices
have already been demonstrated to offer significant
performance improvements[3-5]. The purpose of this work
was to demonstrate that the double gate architecture can be
further enhanced with the use of undoped channels and metal
gate interconnects reducing some of the causes of
performance variation but without changing the material
properties of the critical gate dielectric to gate electrode
interface from traditional integrations. This device structure
consists of a FinFET type channel region (Fig 1.a) but
wrapped on both sides with poly silicon spacers in the gate
region, these spacer gates are doped differently with n+ and
p+ dopants. The spacers are then tied together with a
combination of metals and polysilicon layers (Fig 1.b). The
channel is undoped to keep threshold variations minimal
from dopant fluctuations[6] and avoid mobility degradation.
Defining the gate on a gradual ramped spacer makes
lithography and etch over tall structures easier (Fig 2.). The
option to dope the gate electrodes with various dopant species
on either side of the channel and keep the dopants from crossmigration allows for wide range of Vt adjustment . The
device has thick nitride on top of the channel region and
metal over the polysilicon spacer gates. This allows doping
the very tall source/drain regions with deep high energy
implants without doping the gate and channel region.
Process Integration.
The process steps used to form this structure does not involve
any additional masking steps, the same gate structure can be
used for NMOS and PMOS structures. The Silicon active
region consists of silicon fins with nitride on top these formed
using an etch and trim process on Silicon on Insulator wafers.
The channel has been trimmed down to 30nm thickness and
are 1000A tall. Gate oxide of 24A is grown over this.
Polysilicon gate spacer regions are formed over this channel
and two sides are doped N+ and P+ by angled implants. Due
to isolated spacers the dopants can be driven using thermal
anneals without cross migration of dopants from one side to
another like structures that are prone to possibility of crossmigration [5]. This is followed by deposition of metal and
polysilicon stack. The metal gate is now patterned over these
poly silicon spacers. After etching the stack of metal and
polysilcon and removal of nitride over the channel regions,
source/drain implants and silicidation is then pursued by
standard process to fabricate this device structure as
illustrated in Fig. 3.
P+
Fig 1a: Isolated N+/P+ Strapped structure, Fig 1 b: Cross sectional through the gate and channel
Fig 2: Device showing the smooth line edges of the Metal
gate regions over polysilicon spacer gates.
Fig 3. Cross sectional view of the device structure.
Electrical Characteristics
Fig. 4a shows long channel Id-Vg characteristics of a device
with 0.25µm gate length. This device shows 80mV/decade
sub threshold slope with a linear Vt of 0.14V. We observed
that the subthreshold leakage for gate voltage less than 0.1V
is dominated by gate leakage based on gate leakage
measurement. The enhanced gate leakage is due to quality of
the oxide edges, which could be further improved, with reoxidation of the edges damaged during etch. The
performance of scaled-down 0.1µm device with a different
n+/p+ gate doping is depicted in Fig. 4b.
Fig.4a: Id Vg for Lgate=0.25µm ,Fig 4b: Id-Vg Lgate=0.1µm
This device shows weaker short-channel control and
degraded SS due to the relatively larger body and oxide
thickness to gate length ratio. The linear subthreshold slope
of this device is measured to be 94mV/decade. The Vt of
this device is 0.3V and the Ion is 190µA/ µm and Ioff is
0.5µA/ µm at 1.2V. The Id-Vd characteristics are as shown
in Fig 5.
The Ion is limited by the resistance in the extension regions
as shown by the bunching of the curves at Vd=1.2Vand Vd =
1.5V, this can be improved substantially by optimizing the
extension with selective epitaxy, the gate leakage can be
reduced more by optimizing the oxidation after etch to
reduce edge etch damage. The Short channel effects can be
controlled by going to higher gate-length to channel + gate
dielectric thickness.
Conclusions
A new device structure that takes advantage of the double
gate and extends its features has been demonstrated. Typical
undoped channel integrations of these double gate structures
lead to depletion mode transistors; previously enhancement
mode transistors have been demonstrated with doped
channels[3], or mid-gap gates such as silicided gate
electrodes[5]. New gate metals and mid-gap gate materials at
the oxide interface offer limited control of threshold voltage
and not well understood silicide oxide interfaces [5]. Doped
channels lead to reduction in mobility and threshold voltage
variations due to doping variations. This device structure can
overcome some of these limitations and useful Vt values have
been demonstrated. As CMOS scales down to tens of
nanometer gate lengths, threshold voltages as low as 0.1V
will become necessary, making Vt variation specifications
more stringent. Hence dopant fluctuations in the channel will
become unacceptable. The demonstrated gate stack consists
of well understood materials at the gate dielectric and gate
electrode interface using silicon-dioxide and doped
polysilicon, but the novel gate electrodes comprising of two
isolated regions doped N+/P+ on either side of the channel
region prevents dopant redistribution and enables fixing the
Vt accurately across a wide range for various applications. A
new metal scheme for the gate interconnects that is then
capped with polysilicon and the etch process necessary to
realize this structure has been developed. This allows for
lower interconnect resistance and also allows for traditional
subsequent processing with minimal exposure of the new
metal gate regions. The entire structure does not use any
additional masking steps. Since a common gate can be used
for NMOS and PMOS it can save multiple masking steps that
involve pre-doping the gate. Additional masks can be used to
have multiple Vt devices by varying the dopants in the poly
silicon regions across a wide range than traditionally possible
without doping the channel or changing the gate dielectric.
This novel structure has potential to be used in various
mainstream applications.
Acknowledgements
The Motorola Dan Noble Center for processing the devices
and developing the process modules
References
[1] D. Hisamoto et al, IEEE TED, Vol.38. p 1419-1424,1991
[2] H-S-P. Wong et al. IEDM Tech Dig., 1997 p 427-430
[3} F-L Yang et al, IEDM Tech Dig, 2002, p 255-258
[4] J. Kedzierski et al, IEDM 2001, p 437-440
[5] J. Kedzierski et al, IEDM 2002 , p 247-250
[6] A. Thean et al, IEEE 2002 Silicon Nanoelect. Work., p 25
Fig 5. Id-Vd curves for device with Lgate = 0.1 µm
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