Nancy M. Zelick

Tri-Gate Transistor Architecture with High-k Gate Dielectrics, Metal Gates and Strain Engineering

We have combined the benefits of the fully depleted tri-gate transistor architecture with high-k gate dielectrics, metal gate electrodes and strain engineering. High performance NMOS and PMOS trigate transistors are demonstrated with IDSAT=1.4 mA/mum and 1.1 mA/mum respectively (IOFF=100nA/mum, VCC =1.1V and LG=40nm) with excellent short channel effects (SCE)-DIBL and subthreshold swing, DeltaS. The contributions of strain, the lang100rang vs. lang110rang substrate orientations, high-k gate dielectrics, and low channel doping are investigated for a variety of channel dimensions and FIN profiles. We observe no evidence of early parasitic corner transistor turn-on in the current devices which can potentially degrade ION-IOFF and DeltaS

High mobility Si/SiGe strained channel MOS transistors with HfO/sub 2//TiN gate stack

We integrate a strained Si channel with HfO/sub 2/ dielectric and TiN metal gate electrode to demonstrate NMOS transistors with electron mobility better than the universal mobility curve for SiO/sub 2/, inversion equivalent oxide thickness of 1.4 nm (EOT=1 nm), and with three orders of magnitude reduction in gate leakage. To understand the physical mechanism that improves the inversion electron mobility at the HfO/sub 2//strained Si interface, we measure mobility at various temperatures and extract the various scattering components.

High mobility strained germanium quantum well field effect transistor as the p-channel device option for low power (Vcc = 0.5 V) III–V CMOS architecture

In this article we demonstrate a Ge p-channel QWFET with scaled TOXE = 14.5Å and mobility of 770 cm2/V*s at ns =5×1012 cm−2 (charge density in the state-of-the-art Si transistor channel at Vcc = 0.5V). For thin TOXE < 40 Å, this represents the highest hole mobility reported for any Ge device and is 4× higher than state-of-the-art strained silicon. The QWFET architecture achieves high mobility by incorporating biaxial strain and eliminating dopant impurity scattering. The thin TOXE was achieved using a Si cap and a low Dt transistor process, which has a low oxide interface Dit. Parallel conduction in the SiGe buffer was suppressed using a phosphorus junction layer, allowing healthy subthreshold slope in Ge QWFET for the first time. The Ge QWFET achieves an intrinsic Gmsat which is 2× higher than the InSb p-channel QWFET [3]. These results suggest the Ge QWFET is a viable p-channel option for non-silicon CMOS.