Abstract:Extended x-ray-absorption fine-structure (EXAFS) of copper has been measured from 4 to 500 K and analyzed by the cumulant method, to check the effectiveness of EXAFS as a probe of local dynamics and thermal expansion. The comparison between parallel mean square relative displacements (MSRD) of the first four coordination shells has allowed detecting a significant deviation from a pure Debye behavior. The firstshell EXAFS thermal expansion is larger than the crystallographic one: the difference has allowed eval… Show more
“…10,16 As a first procedure, the ratio method 7,20,21 has been utilized for the first coordination shell, whose contribution can be neatly isolated ( Figure 2) and where MS effects are absent. For each of the two sets of measurements (Ga and As edges), the first-shell EXAFS signals have been obtained by Fourier back-transform of the corresponding peaks in r-space (Fig.…”
Section: Discussionmentioning
confidence: 99%
“…More recently, the difference between the thermal expansions measured by EXAFS and by Bragg diffraction in crystals was experimentally detected, leading to the evaluation of the perpendicular MSRD; the role of the third cumulant was clarified too. 9,10 a) Permanent address: Ain Shams University, Cairo, Egypt. b) Author to whom correspondence should be addressed.…”
“…10,16 As a first procedure, the ratio method 7,20,21 has been utilized for the first coordination shell, whose contribution can be neatly isolated ( Figure 2) and where MS effects are absent. For each of the two sets of measurements (Ga and As edges), the first-shell EXAFS signals have been obtained by Fourier back-transform of the corresponding peaks in r-space (Fig.…”
Section: Discussionmentioning
confidence: 99%
“…More recently, the difference between the thermal expansions measured by EXAFS and by Bragg diffraction in crystals was experimentally detected, leading to the evaluation of the perpendicular MSRD; the role of the third cumulant was clarified too. 9,10 a) Permanent address: Ain Shams University, Cairo, Egypt. b) Author to whom correspondence should be addressed.…”
“…The first term in the sum of ␦R j,L s ͑k͒ is customarily used and expresses the difference between the real and effective first cumulants that correspond to the real and effective average values of the radial distribution. It has been pointed out by Fornasini et al 26 that disorder perpendicular to the scattering path also affects the average distance measured by EXAFS. This is taken into account by the second term ␦R j,Ќ in the argument of the sin function using the approximation…”
Section: ͑8͒mentioning
confidence: 97%
“…In Ref. 26 experimental values of Ќ 2 / ʈ 2 for the first shell of copper were determined and resulted in values larger than 2 and smaller than 3. Considering the first scattering path in Fe with R 1 = 2.470 Å at T = 295 K, for example, the cumulant correction yields 0.011 Å and the correction term due to perpendicular vibrations yields 0.002 Å.…”
Extended x-ray absorption fine structure ͑EXAFS͒ data and magnetic EXAFS ͑MEXAFS͒ data were measured at two temperatures ͑180 and 296 K͒ in the energy region of the overlapping L-edges of bcc Fe grown on a V͑110͒ crystal surface. In combination with a Bayes-Turchin data analysis procedure these measurements enable the exploration of local crystallographic and magnetic structures. The analysis determined the atomiclike background together with the EXAFS parameters which consisted of ten shell radii, the Debye-Waller parameters, separated into structural and vibrational components, and the third cumulant of the first scattering path. The vibrational components for 97 different scattering paths were determined by a two parameter forcefield model using a priori values adjusted to Born-von Karman parameters of inelastic neutron scattering data. The investigations of the system Fe/ V͑110͒ demonstrate that the simultaneous fitting of atomic background parameters and EXAFS parameters can be performed reliably. Using the L 2 -and L 3 -components extracted from the EXAFS analysis and the rigid-band model, the MEXAFS oscillations can only be described when the sign of the exchange energy is changed compared to the predictions of the Hedin Lundquist exchange and correlation functional.
“…In order to extract thermal and structural parameters of NPG from EXAFS data we applied correlated Einstein model 27 that proved effective in many previous studies of bulk 28,29 and nanoscale [30][31][32][33] metals. In this model, parameters 0 k and 3 k of the anharmonic potential, ( )…”
We measured the thermal expansion coefficient and Debye temperature of nanoporous gold (NPG) using Extended X-ray Absorption Fine Structure technique. Reduction of the nearest neighbor distances in NPG by ca. 0.01 Å compared to the bulk gold was attributed to the surface tension caused, in turn, by the finite size effect of the NPG ligaments. We also obtained that the Debye temperature in NPG is 5% lower than in bulk gold. We interpreted these observations in the framework of a bimodal distribution of surface and bulk bonds with different values of Debye temperature. The surface bonds with low Debye temperature extend within ca. 4 layers of Au atoms located on the pore surface, in a good agreement with prior resistivity measurements and theoretical predictions. 63.22.Dc, 61.05.cj, 65.40.De,
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