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1.
J Chem Phys ; 152(3): 034304, 2020 Jan 21.
Artículo en Inglés | MEDLINE | ID: mdl-31968971

RESUMEN

For the inelastic electron scattering of atoms and molecules, a consensus has been reached that the first Born approximation is easily approached by decreasing the momentum transfer at the same impact electron energy or increasing the impact electron energy at the same momentum transfer. Although this consensus is applicable for the elastic electron scattering of most atoms and molecules, it is violated for helium where the experimental differential cross sections deviate from the first Born approximation prediction gradually with the decrease of squared momentum transfer at the same impact electron energy. Since this anomalous phenomenon was observed more than 40 years ago, the intrinsic mechanism is not explicit. In the present work, using the high-resolution x-ray scattering, we isolate the scattering contribution from the nucleus and directly obtain the pure electronic structure of helium. Then, the anomalous asymptotic behavior of the elastic electron scattering of helium has been elucidated, i.e., in the small squared momentum transfer region, the scattering contribution from the target's electrons is counteracted by the one from the atomic nucleus, which results in the residual contribution beyond the first Born approximation being drastically enlarged.

2.
Chemistry ; 16(36): 11064-71, 2010 Sep 24.
Artículo en Inglés | MEDLINE | ID: mdl-20690117

RESUMEN

We report a systematic investigation on the structural and electronic effects of carbon-supported Pt(x)Pd(1-x) bimetallic nanoparticles on the oxygen reduction reaction (ORR) and methanol oxidation reaction (MOR) in acid electrolyte. Pt(x)Pd(1-x)/C nanocatalysts with various Pt/Pd atomic ratios (x=0.25, 0.5, and 0.75) were synthesized by using a borohydride-reduction method. Rotating-disk electrode measurements revealed that the Pt(3)Pd(1)/C nanocatalyst has a synergistic effect on the ORR, showing 50% enhancement, and an antagonistic effect on the MOR, showing 90% reduction, relative to JM 20 Pt/C on a mass basis. The extent of alloying and Pt d-band vacancies of the Pt(x)Pd(1-x)/C nanocatalysts were explored by extended X-ray absorption fine-structure spectroscopy (EXAFS) and X-ray absorption near-edge structure spectroscopy (XANES). The structure-activity relationship indicates that ORR activity and methanol tolerance of the nanocatalysts strongly depend on their extent of alloying and d-band vacancies. The optimal composition for enhanced ORR activity is Pt(3)Pd(1)/C, with high extent of alloying and low Pt d-band vacancies, owing to favorable O-O scission and inhibited formation of oxygenated intermediates. MOR activity also shows structure dependence. For example, Pt(1)Pd(3)/C with Pt(rich-core)Pd(rich-shell) structure possesses lower MOR activity than the Pt(3)Pd(1)/C nanocatalyst with random alloy structure. Herein, extent of alloying and d-band vacancies reveal new insights into the synergistic and antagonistic effects of the Pt(x)Pd(1-x)/C nanocatalysts on surface reactivity.

3.
J Synchrotron Radiat ; 16(Pt 1): 97-104, 2009 Jan.
Artículo en Inglés | MEDLINE | ID: mdl-19096180

RESUMEN

At the National Synchrotron Radiation Research Center (NSRRC), which operates a 1.5 GeV storage ring, a dedicated small-angle X-ray scattering (SAXS) beamline has been installed with an in-achromat superconducting wiggler insertion device of peak magnetic field 3.1 T. The vertical beam divergence from the X-ray source is reduced significantly by a collimating mirror. Subsequently the beam is selectively monochromated by a double Si(111) crystal monochromator with high energy resolution (DeltaE/E approximately 2 x 10(-4)) in the energy range 5-23 keV, or by a double Mo/B4C multilayer monochromator for 10-30 times higher flux ( approximately 10(11) photons s(-1)) in the 6-15 keV range. These two monochromators are incorporated into one rotating cradle for fast exchange. The monochromated beam is focused by a toroidal mirror with 1:1 focusing for a small beam divergence and a beam size of approximately 0.9 mm x 0.3 mm (horizontal x vertical) at the focus point located 26.5 m from the radiation source. A plane mirror installed after the toroidal mirror is selectively used to deflect the beam downwards for grazing-incidence SAXS (GISAXS) from liquid surfaces. Two online beam-position monitors separated by 8 m provide an efficient feedback control for an overall beam-position stability in the 10 microm range. The beam features measured, including the flux density, energy resolution, size and divergence, are consistent with those calculated using the ray-tracing program SHADOW. With the deflectable beam of relatively high energy resolution and high flux, the new beamline meets the requirements for a wide range of SAXS applications, including anomalous SAXS for multiphase nanoparticles (e.g. semiconductor core-shell quantum dots) and GISAXS from liquid surfaces.

4.
Langmuir ; 23(10): 5802-9, 2007 May 08.
Artículo en Inglés | MEDLINE | ID: mdl-17425346

RESUMEN

The chemical state and formation mechanism of Pt-Ru nanoparticles (NPs) synthesized by using ethylene glycol (EG) as a reducing agent and their stability have been examined by in situ X-ray absorption spectroscopy (XAS) at the Pt LIII and Ru K edges. It appears that the reduction of Pt(IV) and Ru(III) precursor salts by EG is not a straightforward reaction but involves different intermediate steps. The pH control of the reaction mixture containing Pt(IV) and Ru(III) precursor salts in EG to 11 led to the reduction of Pt(IV) to Pt(II) corresponding to [PtCl4](2-) whereas Ru(III)Cl3 is changed to the [Ru(OH)6](3-) species. Refluxing the mixture containing [PtCl4](2-) and [Ru(OH)6](3-) species at 160 degrees C for 0.5 h produces Pt-Ru NPs as indicated by the presence of Pt and Ru in the first coordination shell of the respective metals. No change in XAS structural parameters is found when the reaction time is further increased, indicating that the Pt-Ru NPs formed are extremely stable and less prone to aggregation. XAS structural parameters suggest a Pt-rich core and a Ru-rich shell structure for the final Pt-Ru NPs. Due to the inherent advantages of the EG reduction method, the atomic distribution and alloying extent of Pt and Ru in the Pt-Ru NPs synthesized by the EG method are higher than those of the Pt-Ru/C NPs synthesized by a modified Watanabe method.

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