2017
DOI: 10.1246/cl.170423
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Polarization-dependent Total Reflection Fluorescence X-ray Absorption Fine Structure (PTRF-XAFS) Studies on the Structure of a Pt Monolayer on Au(111) Prepared by the Surface-limited Redox Replacement Reaction

Abstract: We studied the initial stage of a Pt monolayer produced by surface-limited redox replacement (SLRR) using polarizationdependent total reflection fluorescence X-ray absorption fine structure (PTRF-XAFS). Different from the widely accepted understanding that metallic monolayer islands are formed, our XAFS showed that the Pt monolayer, initially present on the Au(111) substrate, was mainly in the form of a planar [PtCl 4 ] 2¹ complex with its molecular plane parallel to Au(111). This result provides a new ins… Show more

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Cited by 10 publications
(17 citation statements)
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References 38 publications
(31 reference statements)
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“…Extended X-ray absorption fine structure (extended XAFS or EXAFS) spectroscopy is a suitable and widely-used method to investigate the local atomic structures of fuel-cell catalysts because of its atomic selectivity and applicability to nanoparticles under electrochemical environments [6]. However, in case of Pt-Au system, it is difficult to obtain a Pt L 3 -edge EXAFS sufficient for its analysis due to the interference between Pt and Au, which are only separated by~350 eV, so that Au L 3 -edge appears at~9.6 Å −1 in Pt L 3 -edge EXAFS [7,8]. Although the problem can be solved by measuring K-edge XAFS, where Pt and Au K-edges are separated by 2300 eV [9,10], the information in the long-range order is limited by the lifetime broadening, and Pt L 3 -edge EXAFS measurement is preferable.…”
Section: Introductionmentioning
confidence: 99%
“…Extended X-ray absorption fine structure (extended XAFS or EXAFS) spectroscopy is a suitable and widely-used method to investigate the local atomic structures of fuel-cell catalysts because of its atomic selectivity and applicability to nanoparticles under electrochemical environments [6]. However, in case of Pt-Au system, it is difficult to obtain a Pt L 3 -edge EXAFS sufficient for its analysis due to the interference between Pt and Au, which are only separated by~350 eV, so that Au L 3 -edge appears at~9.6 Å −1 in Pt L 3 -edge EXAFS [7,8]. Although the problem can be solved by measuring K-edge XAFS, where Pt and Au K-edges are separated by 2300 eV [9,10], the information in the long-range order is limited by the lifetime broadening, and Pt L 3 -edge EXAFS measurement is preferable.…”
Section: Introductionmentioning
confidence: 99%
“…In the XAFS spectrum without the BCLA, strong Au L X-ray fluorescence appeared above 11900 eV (the Au L 3 edge). Even under the total reflection conditions, X-rays could penetrate the bulk and excite the Au edge (Yuan et al, 2017). Fig.…”
Section: Resultsmentioning
confidence: 99%
“…By combining with the polarization dependence, we can obtain the three-dimensional structure in PTRF-XAFS. In the liquid-solid interface system, PTRF-XAFS requires a less than 1 mm thick solution to reduce absorption and scattering of the solution (Tamura et al, 2000;Masuda et al, 2016;Yuan et al, 2017Yuan et al, , 2018. However, such a thin liquid layer hinders material diffusion and cannot follow the electrochemical process continuously.…”
Section: Comparison With Other In Situ Surface Xafs Techniquesmentioning
confidence: 99%
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“…XAFS Measurements and Analysis. To eliminate oxygen contamination, an in situ polychloro-trifluoroethylene (PCTFE) XAFS cell 27 was assembled in the glovebox. A Mylar film with thickness of 6 μm was used as the X-ray window.…”
Section: ■ Experimental Sectionmentioning
confidence: 99%