Fabrication and analysis of deep submicron strained-Si n-MOSFET's
TL;DR: In this paper, deep submicron strained-Si n-MOSFETs were fabricated on strained Si/relaxed Si/sub 0.8/Ge/sub sub 0.2/ heterostructures to yield well matched channel doping profiles after processing, allowing comparison of strained and unstrained Si surface channel devices.
Abstract: Deep submicron strained-Si n-MOSFETs were fabricated on strained Si/relaxed Si/sub 0.8/Ge/sub 0.2/ heterostructures. Epitaxial layer structures were designed to yield well-matched channel doping profiles after processing, allowing comparison of strained and unstrained Si surface channel devices. In spite of the high substrate doping and high vertical fields, the MOSFET mobility of the strained-Si devices is enhanced by 75% compared to that of the unstrained-Si control devices and the state-of-the-art universal MOSFET mobility. Although the strained and unstrained-Si MOSFETs exhibit very similar short-channel effects, the intrinsic transconductance of the strained Si devices is enhanced by roughly 60% for the entire channel length range investigated (1 to 0.1 /spl mu/m) when self-heating is reduced by an ac measurement technique. Comparison of the measured transconductance to hydrodynamic device simulations indicates that in addition to the increased low-field mobility, improved high-field transport in strained Si is necessary to explain the observed performance improvement. Reduced carrier-phonon scattering for electrons with average energies less than a few hundred meV accounts for the enhanced high-field electron transport in strained Si. Since strained Si provides device performance enhancements through changes in material properties rather than changes in device geometry and doping, strained Si is a promising candidate for improving the performance of Si CMOS technology without compromising the control of short channel effects.
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Patent•
03 Jan 2005TL;DR: In this paper, a method of fabricating a semiconductor structure is described, which includes a substrate, an insulating layer, a relaxed SiGe layer where the Ge composition is larger than approximately 15%, and a device layer selected from a group consisting of, but not limited to, strained-Si, relaxed Si1-yGey layer, strained Si 1-zGez layer, Ge, GaAs, III-V materials, and II-VI materials, where Ge compositions y and z are values between 0 and 1.
Abstract: A method of fabricating a semiconductor structure. According to one aspect of the invention, on a first semiconductor substrate, a first compositionally graded Si1-xGex buffer is deposited where the Ge composition x is increasing from about zero to a value less than about 20%. Then a first etch-stop Si1-yGey layer is deposited where the Ge composition y is larger than about 20% so that the layer is an effective etch-stop. A second etch-stop layer of strained Si is then grown. The deposited layer is bonded to a second substrate. After that the first substrate is removed to release said first etch-stop S1-yGey layer. The remaining structure is then removed in another step to release the second etch-stop layer. According to another aspect of the invention, a semiconductor structure is provided. The structure has a layer in which semiconductor devices are to be formed. The semiconductor structure includes a substrate, an insulating layer, a relaxed SiGe layer where the Ge composition is larger than approximately 15%, and a device layer selected from a group consisting of, but not limited to, strained-Si, relaxed Si1-yGey layer, strained Si1-zGez layer, Ge, GaAs, III-V materials, and II-VI materials, where Ge compositions y and z are values between 0 and 1.
16 citations
01 Sep 2007
TL;DR: In this article, the authors review recent developments of the Monte Carlo approach to the simulation of semi-classical carrier transport in nano-MOSFETs, with particular focus on the inclusion of quantum-mechanical effects in the simulation (using either the Multi-Subband approach or quantum corrections to the electrostatic potential) and on the numerical stability issues related to the coupling of the transport with the Poisson equation.
Abstract: In this paper, we review recent developments of the Monte Carlo approach to the simulation of semi-classical carrier transport in nano-MOSFETs, with particular focus on the inclusion of quantum-mechanical effects in the simulation (using either the Multi-Subband approach or quantum corrections to the electrostatic potential) and on the numerical stability issues related to the coupling of the transport with the Poisson equation. Selected applications are presented, including the analysis of quasi-ballistic transport, the determination of the RF characteristics of deca-nanometric MOSFETs, and the study of non- conventional device structures and channel materials.
16 citations
TL;DR: In this paper, the authors developed a novel CMOS architecture that uses mechanical tensile stress, induced by the Si nitride-capping layer, together with the pseudomorphic compressive stress in SiGe layer to improve the drive current of both n- and pMOSFETs simultaneously.
Abstract: We developed a novel CMOS architecture that uses mechanical tensile stress, induced by the Si nitride-capping layer, together with the pseudomorphic compressive stress in SiGe layer to improve the drive current of both n- and pMOSFETs simultaneously. The unique advantage of this process flow is that on the same wafer, individual MOSFET performance can be adjusted independently to their optimum due to the separation process for two type devices. It is found that n- and pMOSFETs in the novel CMOS architecture behaved better in performance, not only a higher drain-to-source saturation current but also higher transconductance with wide gate voltage swing, than the Si-control devices, thus making this flow to show a great flexibility for developing next-generation high-performance CMOS.
16 citations
Patent•
29 Jun 2006TL;DR: In this paper, a multi-layered reflective mirror formed of spaced-apart plate-shaped empty space patterns formed within a substrate is disclosed, and a plurality of plateshaped empty spaces patterns are formed by drilling holes in the substrate and annealing the substrate to form the spaced-array empty spaces.
Abstract: A multi-layered reflective mirror formed of spaced-apart plate-shaped empty space patterns formed within a substrate is disclosed. The plurality of plate-shaped empty space patterns are formed by drilling holes in the substrate and annealing the substrate to form the spaced-apart plate-shaped empty space patterns.
15 citations
TL;DR: In this article, the authors mapped the active layer of a silicon-on-insulator substrate induced by through-silicon via (TSV) structures using x-ray microbeam diffraction.
Abstract: Strain distributions within the active layer of a silicon-on-insulator substrate induced by through-silicon via (TSV) structures were mapped using x-ray microbeam diffraction. The interaction region of the out-of-plane strain, e33, from a TSV feature containing copper metallization extended approximately 6 μm from the TSV outer edge for circular and annular geometries. Measurements conducted on identical TSV structures without copper reveal that strain fields generated by the liner materials extend a similar distance and with comparable magnitude as those with copper. FEM-based simulations show the total interaction region induced by the TSV can extend farther than that of e33.
15 citations
References
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IBM1
TL;DR: In this article, the authors compute the band structure and shear deformation potentials of strained Si, Ge, and SiGe alloys, and fit the theoretical results to experimental data on the phonon-limited carrier mobilities in bulk Si and Ge.
Abstract: Using nonlocal empirical pseudopotentials, we compute the band structure and shear deformation potentials of strained Si, Ge, and SiGe alloys. Fitting the theoretical results to experimental data on the phonon‐limited carrier mobilities in bulk Si and Ge, the dilatation deformation potential Ξd is found to be 1.1 eV for the Si Δ minima, −4.4 eV for the Ge L minima, corresponding to a value for the valence band dilatation deformation potential a of approximately 2 eV for both Si and Ge. The optical deformation potential d0 is found to be 41.45 and 41.75 eV for Si and Ge, respectively. Carrier mobilities in strained Si and Ge are then evaluated. The results show a large enhancement of the hole mobility for both tensile and compressive strain along the [001] direction, but only a modest enhancement (approximately 60%) of the electron mobility for tensile biaxial strain in Si. Finally, from a fit to carrier mobilities in relaxed SiGe alloys, the effective alloy scattering potential is determined to be about 0...
1,500 citations
TL;DR: In this paper, the inversion layer mobility in n-and p-channel Si MOSFETs with a wide range of substrate impurity concentrations (10/sup 15/ to 10/sup 18/ cm/sup -3/) was examined.
Abstract: This paper reports the studies of the inversion layer mobility in n- and p-channel Si MOSFET's with a wide range of substrate impurity concentrations (10/sup 15/ to 10/sup 18/ cm/sup -3/). The validity and limitations of the universal relationship between the inversion layer mobility and the effective normal field (E/sub eff/) are examined. It is found that the universality of both the electron and hole mobilities does hold up to 10/sup 18/ cm/sup -3/. The E/sub eff/ dependences of the universal curves are observed to differ between electrons and holes, particularly at lower temperatures. This result means a different influence of surface roughness scattering on the electron and hole transports. On substrates with higher impurity concentrations, the electron and hole mobilities significantly deviate from the universal curves at lower surface carrier concentrations because of Coulomb scattering by the substrate impurity. Also, the deviation caused by the charged centers at the Si/SiO/sub 2/ interface is observed in the mobility of MOSFET's degraded by Fowler-Nordheim electron injection. >
1,389 citations
TL;DR: In this paper, the thermal resistivity, Seebeck coefficient, electrical resistivity and Hall mobility of GeSi alloys have been measured throughout the GeSi alloy system as functions of impurity concentration in the range 2×1018−4×1020cm−3, and of temperature in range 300°-1300°K.
Abstract: The thermal resistivity, Seebeck coefficient, electrical resistivity, and Hall mobility of Ge‐Si alloys have been measured throughout the Ge‐Si alloy system as functions of impurity concentration in the range 2×1018−4×1020cm−3, and of temperature in the range 300°–1300°K. A qualitative interpretation of these properties is given. For power conversion, boron and phosphorus were found to be useful p‐type and n‐type impurities, respectively, because of their high solid solubilities. At 1200°K, the maximum values of the dimensionless figure of merit zT were 0.8 for p‐type Ge0.15‐Si0.85 alloy doped to 2.1×1020cm−3 holes, and 1.0 for n‐type Ge0.15‐Si0.85 alloy doped to 2.7×1020cm−3 electrons. The maximum over‐all efficiency of a stable generator operating between 300°–1200°K, using the best p‐type and n‐type materials was computed to be 10%.
556 citations
TL;DR: In this paper, the authors investigated the phonon-limited mobility of strained Si metal-oxide-semiconductor field effect transistors (MOSFETs) through theoretical calculations including two-dimensional quantization.
Abstract: The phonon‐limited mobility of strained Si metal–oxide–semiconductor field‐effect transistors (MOSFETs) fabricated on a SiGe substrate is investigated through theoretical calculations including two‐dimensional quantization, and compared with the mobility of conventional (unstrained) Si MOSFETs. In order to match both the mobility of unstrained Si MOSFETs and the mobility enhancement in strained Si MOSFETs, it is necessary to increase the coupling of electrons in the two‐dimensional gas with intervalley phonons, compared to the values used in conventional models. The mobility enhancement associated with strain in Si is attributed to the following two factors: the suppression of intervalley phonon scattering due to the strain‐induced band splitting, and the decrease in the occupancy of the fourfold valleys which exhibit a lower mobility due to the stronger interaction with intervalley phonons. While the decrease in the averaged conductivity mass, caused by the decrease in the occupancy of the fourfold valle...
454 citations
TL;DR: In this paper, the authors developed a technique for measuring the thermal conductivity of silicon-on-insulator (SOI) transistors and provided data for layers in wafers fabricated using bond-and-etch-back (BESOI) technology.
Abstract: Self heating diminishes the reliability of silicon-on-insulator (SOI) transistors, particularly those that must withstand electrostatic discharge (ESD) pulses. This problem is alleviated by lateral thermal conduction in the silicon device layer, whose thermal conductivity is not known. The present work develops a technique for measuring this property, and provides data for layers in wafers fabricated using bond-and-etch-back (BESOI) technology. The room-temperature thermal conductivity data decrease with decreasing layer thickness, d s , to a value nearly 40 percent less than that of bulk silicon for d s = 0.42 μm, The agreement of the data with the predictions of phonon transport analysis between 20 and 300 K strongly indicates that phonon scattering on layer boundaries is responsible for a large part of the reduction. The reduction is also due in part to concentrations of imperfections larger than those in bulk samples. The data show that the buried oxide in BESOI wafers has a thermal conductivity that is nearly equal to that of bulk fused quartz. The present work will lead to more accurate thermal simulations of SOI transistors and cantilever MEMS structures.
358 citations