Abstract:
Semiconductor industry is approaching towards the end of technology
roadmap as the device dimensions are shrinking. Novel device structures are being
investigated to follow the scaling trends of International Technology Roadmap for
Semiconductors (ITRS). Various modifications at circuit level have also been carried
out in order to meet area constraints and power budgeting limitations. Due to
downscaling of single gate bulk MOSFET, power consumption increases due to short
channel effects (SCEs) including threshold voltage roll-off and subthreshold slope
degradation. Such effects increase the leakage current associated with the device
hence increases the power consumption. Hence, emerging research device (ERD)
community is looking for such a device with low threshold voltage, low leakage and
high performance. This results in multiple gate structure such as Double Gate (DG)
MOSFET.
Double Gate MOSFETs are classified broadly into two categories as;
Asymmetric Double Gate (ASDG) MOSFET: asymmetric nature of the device can be
obtained with different work functions for both front and back gates, different
insulator layer thicknesses and different gate potentials applied on both the gates.
Symmetric Double Gate (SDG) MOSFET: a symmetric type DG MOSFET with both
the gates having identical work functions, identical insulator layer thicknesses and
same applied gate potentials. Another class of DG MOSFET is Metal Gate Double
Gate (MGDG) MOSFET, which is used for ultra low power consumption circuits
with gate as metal and with intrinsic channel doping. MGDG offers various
advantages: metal gate eliminates poly depletion effect and eliminates threshold
voltage fluctuations. Subthreshold current is reduced due to less DIBL and reduced
short channel effects, because of absence of bulk charge in channel. Hence negligible
surface electric field causes lower gate to channel leakage and intrinsic body doping
eliminates random dopant fluctuation. Further, electric field at the edges as well as
interface is reduced which results into a decrease in edge direct tunneling current
[116]. Midgap metal gates are easier from fabrication perspective but reduces the
performance hence dual metal gates are required for improved performance. In our
current work, we have proposed a dual metal gate device with ultra thin Aluminum
Nitride (A1NX) buffer layer with Hafnium (Hf) as gate metal with work functions of
4.4 eV for n-channel device. Because of equal applied potentials on both the gates,
symmetric word is associated with the proposed device, known as Metal Gate
Symmetric Double Gate (MG-SDG) MOSFET.
One dimensional potential modeling of single of double gate MOSFET is not
enough to explain its various physical facts within the device in nanoscale regime. At
extremely low dimensions, electric field in both longitudinal and transverse directions
becomes substantially large. Hence, two dimensional (2D) device modeling is
required to enhance the accuracy of the results. 2D models gives a more accurate
result but at the cost of the computation time. Ways and means should be found out
both at modeling as well as architectural level in order to reduce the computation time
without compromising on the accuracy of the result. In this thesis, 2D analytical
potential modeling, inversion charge density modeling and drain current modeling is
carried out for nanoscale MG-SDG MOSFET and Midgap Symmetric Double Gate
(SDG) MOSFET through the evaluation ofquantum surface potential. 2D analytical
potential modeling is carried out first for Asymmetric Double Gate (ASDG)
MOSFET and then modeled for SDG MOSFET with ultra thin body (UTB) device
with boundary values which are based on the physics of the device. Center and
surface potential is modeled analytically in this thesis below threshold voltage while
in the post threshold voltage, it has been modeled using 2D ATLAS device simulator.
Quantum mechanical corrections (QMC) are applied for the purpose of modeling of
potential, inversion charge density and drain current through threshold voltage.
Variation of threshold voltage with various device parameters is evaluated. Variation
of surface potential and inversion charge density is carried out with gate to source
voltage. A shift in surface potential due to Quantum Mechanical (QM) approach is
observed as compared to classical model. Variations of inversion charge density and
drain current are carried out with various device parameters. For the purpose of
verification and validation of our proposed model, we have compared and contrasted
the results obtained through our model and the results obtained through 2D ATLAS
device simulator.
Low leakage devices are required for low power consumption for various
applications. The work function engineering alters the threshold voltage of the nchannel
MG-SDG for low power high performance nanoscale circuit design with
Hf/A1NX as gate metal using both conventional (Si02) and high-k dielectric (Si3N4).
We have chosen Hf/A1NX as gate metal because ofits optimum threshold voltage and
leakage currents. Further, our analysis shows the improvement in the performance due
to reduced threshold voltage and reduction in gate leakage current with Si3N4 as gate
dielectric. We have analytically calculated subthreshold slope and ideality factor for
MG-SDG MOSFET to evaluate the subthreshold current. The electric field modeling
across an insulator layer is carried out for the modeling of gate to channel leakage
current and edge direct tunneling leakage current. The local electric field is modeled
from the developed 2D potential modeling for the estimation of band to band
in
tunneling current. Asubstantial reduction in all the leakage components for the device
under study with respect to currentDG devices is obtained.
It can be appreciated that the devices by themselves don't add to the existing
integration era. But until, a circuit analysis using the proposed devices is undertaken,
the full benefits of integration cannot be captured. Logic and memory circuit design in
nanoscale regime requires control over leakage currents with device level parameter
variations. MGDG MOSFET has been proved to be vital in nanoscale regime for its
leakage reduction with appropriate back gate bias and reduced sensitivity to process
parameter variations. Super coupling effects are considered for evaluating leakage
currents with back gate bias for both conventional (Si02) and high-k dielectric
(S13N4). The proposed DG device/circuit co-design successfully demonstrates the
benefit of using independent gate devices which significantly reduces leakages in
Static Random Access Memory (SRAM) architecture while minimizing the latency
time. Effect of back gate bias on front channel electrical properties is modeled
through variation in front channel threshold voltage. In our design, we typically used
forward biased back gate devices in critical path during active operation to improve
performance and switch to negative back gate bias during standby mode to reduce
leakage. From analysis, it has been found that at aback gate bias of -0.4V, most of the
leakage currents are minimum. Except BTBT current, all leakage currents will
increase monotonically with back gate voltage from -0.4V to 0.4V. But its value
becomes very low as compared to other leakage components. Gate to body
capacitance becomes minimum in DG MOSFET's with intrinsic body, so we can
exploit this feature for minimizing the latency time with back gate bias in MGDG
MOSFET for robust circuit/memory design in nanometer regime. Our analysis shows
that use ofMGDG devices with intrinsic body reduces latency introduced by body
biasing mechanisms for leakage reduction. Hence, we conclude that MGDG
MOSFET can emerge as one of the promising candidate for reducing all leakage
components with minimum body transition time making it efficient for low power and
high performance circuit design in nanoscale regime.