2000
DOI: 10.1016/s0094-5765(00)00026-6
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Life and intelligence in the universe from nanobiological principles: A survey and budget of concepts and perspectives

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“…78 Similarly, the degeneracies of the TR2 and TR3 paths were related to that of the TR1 path in the fit (Table 5). Finally, the third cumulant, σ (3) , was added to the list of variables for the 1NN path to account for the temperaturedependent and, possibly, size-dependent asymmetry of the 1NN pair distance distribution function. Figure 8 presents the theoretical EXAFS fits of the data collected for all the samples and the Pt metal foil at 200 K. The fit results for the coordination numbers of the nearest neighboring shells, first through the fifth, are summarized in the Table 5.…”
Section: Resultsmentioning
confidence: 99%
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“…78 Similarly, the degeneracies of the TR2 and TR3 paths were related to that of the TR1 path in the fit (Table 5). Finally, the third cumulant, σ (3) , was added to the list of variables for the 1NN path to account for the temperaturedependent and, possibly, size-dependent asymmetry of the 1NN pair distance distribution function. Figure 8 presents the theoretical EXAFS fits of the data collected for all the samples and the Pt metal foil at 200 K. The fit results for the coordination numbers of the nearest neighboring shells, first through the fifth, are summarized in the Table 5.…”
Section: Resultsmentioning
confidence: 99%
“…The EXAFS signal, χ(k), which is the sum of all contributions, χ i (k), from groups of atoms that lie at approximately equal distances from the absorbing atom (i.e., the ith shell) was adjusted by applying the EXAFS equation, written in the following extended form: 72 where k is the photoelectron wavenumber, f i eff (k) and δ i (k) are the photoelectron scattering-path amplitude and phase, respectively, S 0 2 is the passive electron reduction factor, R i is the effective half-path-length (which is equal to the interatomic distance for single-scattering paths),σ i 2 (discussed further below) is the mean-square deviation in R i , σ i (3) is the third cumulant, and λ i (k) is the photoelectron mean free path. The computer code FEFFIT was used to fit theoretical EXAFS calculated with FEFF6 to the experimental χ(k) data.…”
Section: Methodsmentioning
confidence: 99%
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