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•
31 Aug 2004TL;DR: In this article, at least two strong bonding regions are defined for a desired bond between a semiconductor membrane and a crystalline semiconductor substrate, separated by a weak bonding region.
Abstract: One aspect of the present invention relates to a method for forming a strained semiconductor structure. In various embodiments, at least two strong bonding regions are defined for a desired bond between a crystalline semiconductor membrane and a crystalline semiconductor substrate. The two strong bonding regions are separated by a weak bonding region. The membrane is bonded to the substrate at a predetermined misorientation. The membrane is pinned to the substrate in the strong bonding regions. The predetermined misorientation provides the membrane in the weak bonding region with a desired strain. In various embodiments, the membrane is bonded to the substrate at a predetermined twist angle to biaxially strain the membrane in the weak bonding region. In various embodiments, the membrane is bonded to the substrate at a predetermined tilt angle to uniaxially strain the membrane in the weak bonding region. Other aspects are provided herein.
41 citations
Patent•
30 Nov 2006TL;DR: In this article, a method for creating a gettering site in a semiconductor wafer is described, in which the wafer undergoes a surface transformation to transform the arrangement of the plurality of holes into a predetermined arrangement of at least one empty space of a predetermined size.
Abstract: One aspect of this disclosure relates to a method for creating a gettering site in a semiconductor wafer. In various embodiments, a predetermined arrangement of a plurality of holes is formed in the semiconductor wafer through a surface of the wafer. The wafer is annealed such that the wafer undergoes a surface transformation to transform the arrangement of the plurality of holes into a predetermined arrangement of at least one empty space of a predetermined size within the wafer to form the gettering site. One aspect relates to a semiconductor wafer. In various embodiments, the wafer includes at least one device region, and at least one gettering region located proximate to the at least one device region. The gettering region includes a precisely-determined arrangement of a plurality of precisely-formed voids that are formed within the wafer using a surface transformation process. Other aspects and embodiments are provided herein.
40 citations
Patent•
21 May 2003TL;DR: In this paper, a method for forming a semiconductor on insulator structure includes providing a glass substrate, providing a silicon wafer, and performing a bonding cut process on the semiconductor wafer and the glass substrate to provide a thin semiconductor layer.
Abstract: A method for forming a semiconductor on insulator structure includes providing a glass substrate, providing a semiconductor wafer, and performing a bonding cut process on the semiconductor wafer and the glass substrate to provide a thin semiconductor layer bonded to the glass substrate. The thin semiconductor layer is formed to a thickness such that it does not yield due to temperature-induced strain at device processing temperatures. An ultra-thin silicon layer bonded to a glass substrate, selected from a group consisting of a fused silica substrate, a fused quartz substrate, and a borosilicate glass substrate, provides a silicon on insulator wafer in which circuitry for electronic devices is fabricated.
40 citations
TL;DR: In this paper, the authors compared the performance of single-and dual-surface channel devices fabricated using 15% Ge content SiGe virtual substrates and found that the compromised performance of the dual-channel devices are attributed to greater interface roughness and increased Ge diffusion resulting from the Si/sub 0.7/Ge/sub 1.3/ buried channel layer.
Abstract: Results comparing strained-Si-SiGe n-channel MOSFET performance of single-and dual-surface channel devices fabricated using 15% Ge content SiGe virtual substrates are presented. Device fabrication used high thermal budget processes and virtual substrates were not polished. Mobility enhancement factors exceeding 1.6 are demonstrated for both single-and dual-channel device architectures compared with bulk-Si control devices. Single-channel devices exhibit improved gate oxide quality, and larger mobility enhancements, at higher vertical effective fields compared with the dual-channel strain-compensated devices. The compromised performance enhancements of the dual-channel devices are attributed to greater interface roughness and increased Ge diffusion resulting from the Si/sub 0.7/Ge/sub 0.3/ buried channel layer.
39 citations
TL;DR: In this paper, a semianalytical model for the energy dispersion of the holes in the inversion layer of pMOS transistors is presented, where wave vector dependence of the energy inside the 2D subbands is described with an analytical, nonparabolic, and anisotropic expression.
Abstract: This paper presents a new semianalytical model for the energy dispersion of the holes in the inversion layer of pMOS transistors. The wave vector dependence of the energy inside the 2-D subbands is described with an analytical, nonparabolic, and anisotropic expression. The procedure to extract the parameters of the model is transparent and simple, and we have used the band structure obtained with the k ldr p method to calibrate the model for silicon MOSFETs with different crystal orientations. The model is validated by calculating several transport-related quantities in the inversion layer of a heavily doped pMOSFET and by systematically comparing the results to the corresponding k ldr p calculations. Finally, we have used the newly developed band-structure model to calculate the effective mobility of pMOS transistors and compare the results with the experimental data. The overall computational complexity of our model is dramatically smaller compared to a fully numerical treatment (such as the k ldr p method); hence, our approach opens new possibilities for the physically based modeling of pMOS transistors.
39 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