Abstract:The band offsets for strained Si 1−x−y Ge x C y layers grown on Si(001) substrate and for strained Si 1−x Ge x layers grown on fully relaxed Si 1−z Ge z virtual substrates are estimated. The hydrostatic strain, the uniaxial strain and the intrinsic chemical effect of Ge and C are considered separately. Unknown material parameters relative to the latter effect are chosen to give the best agreement with the available experimental results for Si 1−x Ge x and Si 1−y C y layers on Si. As a general trend concerning … Show more
“…Therefore, process margin for SiGe HBT fabrication can be relaxed. On the other hand, it has been reported that the bandgap and the band offsets with respect to the conduction band and valence band sensitively varies with C contents and strain in Si 1ÀxÀy Ge x C y films [151][152][153][154][155][156][157][158][159][160][161]. On the basis of the control over the band alignment in the Si 1ÀxÀy Ge x C y hetero structures, Si 1ÀxÀy Ge x C y epitaxial films were applied to channel layers in MOSFET [162,163], high-electron mobility transistor (HEMT), and optical devices [164][165][166].…”
“…Therefore, process margin for SiGe HBT fabrication can be relaxed. On the other hand, it has been reported that the bandgap and the band offsets with respect to the conduction band and valence band sensitively varies with C contents and strain in Si 1ÀxÀy Ge x C y films [151][152][153][154][155][156][157][158][159][160][161]. On the basis of the control over the band alignment in the Si 1ÀxÀy Ge x C y hetero structures, Si 1ÀxÀy Ge x C y epitaxial films were applied to channel layers in MOSFET [162,163], high-electron mobility transistor (HEMT), and optical devices [164][165][166].…”
“…This type of biaxial strain introduces a splitting of degenerate bands [1][2] which results, for both electrons and holes, in smaller in-plane effective mass and reduced intervalley scattering yielding improved transport properties. N-type Si/SiGe modulation-doped FETs (MODFETs) have demonstrated low noise figure and high cut-off and maximum oscillation frequencies [3][4].…”
The electron transport in the two-dimensional gas formed in tensile-strained Si 1-x Ge x /Si/Si 1-x Ge x heterostructures is investigated using Monte Carlo simulation. At first the electron mobility is studied in ungated modulation doped structures. The calculation matches very well the experimental results over a wide range of electron density. The mobility typically varies between 1100 cm 2 /Vs in highly-doped structures and 2800 cm 2 /Vs at low electron density. The mobility is shown to be significantly influenced by the thickness of the spacer layer separating the strained Si channel from the pulse-doped supply layers. Then the electron transport is investigated in a gated modulation-doped structure in which the contribution of parasitic paths is negligible. The mobility is shown to be higher than in comparable ungated structures and dependent on the gate voltage, as a result of the electron density dependence of remote impurity screening.
“…A coherent strain applied along direction ͑001͒ lifts at least partially the degeneracy of conduction and valence bands. 35 In case of tensile strain the energy position of normal ⌬ valleys shifts down, whereas that of parallel valleys shifts up, as illustrated in Fig. 6.…”
Section: Heterojunction Mos Structuresmentioning
confidence: 90%
“…33,34 A similar design of n-type MOSFET requires a tensile strained layer to create a convenient conduction band offset. 35 Two types of heterostructures may be used in this order. Classically, a tensile strain is obtained by growing a Si layer on a Si 1Ϫx Ge x virtual substrate.…”
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