... Weber in Ref [76] as the following ϵ = 50 kcal/mol, σ = 0.20951 nm, A = 7.049556277, (2.8) B = 0.6 0222 45584, p = 4, q = 0, a = 1.80, λ = 21.0, γ = 1.20 The parameter set of SW potential for Ge was ... Ding et al in Ref [80] as the following ϵ = 1.93 eV, σ = 0.2181 nm, A = 7.049556277, (2.9) B = 0.6 0222 45584, p = 4, q = 0, a = 1.80, λ = 31.0, γ = 1.20 These two parameter sets are different in parameter ... threshold are also discussed Finally, we summarize this thesis and give the conclusions in Chapter 22 Chapter Simulation Methods In this chapter, we first introduce the basic principles of molecular...
... 2001, 80 :220 14 Stoney GC: The Tension of Metallic Films Deposited by Electrolysis Proc R Soc Lond A 1909, 32:172 15 Nix WD: Mechanical properties of thin films Metall Trans A 1989, 20 :221 7 16 ... thermal stability of hydrogen in amorphous silicon and germanium J Non-Cryst Solids 1996, 198-200:40 22 Chou YP, Lee SC: Structural, optical, and electrical properties of hydrogenated amorphous silicon...
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... shows two sets of peaks One set consists of the Ž111., 220 and Ž311 peaks of Si which are from the SiNWs The other set consists of the Ž111., 220 and Ž311 peaks of b-SiC which are from the b-SiC ... shows there are two sets of rings One consists of the Ž111., 220 and Ž311 rings of silicon The other corresponds to the Ž111., 220 and Ž311 rings of b-SiC This confirms that the sample is a ... w111x ŽSAED pattern taken from the nanowires The diffraction rings match well with the Ž111., 220 and Ž311 diffraction rings of silicon with a diamond structure Analysis using energy dispersive...
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