Abstract:Semiconducting
oxide nanoparticles are strongly influenced by surface-adsorbed
molecules and tend to generate an insulating depletion layer. The
interface between a noble metal and a semiconducting oxide constructs
a Schottky barrier, interrupting the electron transport. In the case
of a Pt catalyst supported on the semiconducting oxide Nb-doped SnO2 with a fused-aggregate network structure (Pt/Nb-SnO2) for polymer electrolyte fuel cells, the electronic conductivity
increased abruptly with increasing Pt loadin… Show more
“…Kakinuma et al. [ 402 ] reported that the Pt deposited onto Nb‐doped SnO 2 formed a PtSn alloy between the catalyst and the surface, which enhanced the electron transfer to the catalyst by reducing the Schottky‐type barrier. They also reported that the conductivity had a significant dependence on the Pt loading.…”
Polymer electrolyte fuel cells (PEFCs) are a promising replacement for the fossil fuel–dependent automotive and energy sectors. They have become increasingly commercialized in the last decade; however, significant limitations on durability and performance limit their commercial uptake. Catalyst layer (CL) design is commonly reported to impact device power density and durability; although, a consensus is rarely reached due to differences in testing conditions, experimental design, and types of data reported. This is further exacerbated by aspects of CL design such as catalyst support, proton conduction, catalyst, fabrication, and morphology, being significantly interdependent; hence, a wider appreciation is required in order to optimize performance, improve durability, and reduce costs. Here, the cutting‐edge research within the field of PEFCs is reviewed, investigating the effect of different manufacturing techniques, electrolyte distribution, support materials, surface chemistries, and total porosity on power density and durability. These are critically appraised from an applied perspective to inform the most relevant and promising pathways to make and test commercially viable cells. This holistic view of the competing aspects of CL design and preparation will facilitate the development of optimized CLs, especially the incorporation of novel catalyst support materials.
“…Kakinuma et al. [ 402 ] reported that the Pt deposited onto Nb‐doped SnO 2 formed a PtSn alloy between the catalyst and the surface, which enhanced the electron transfer to the catalyst by reducing the Schottky‐type barrier. They also reported that the conductivity had a significant dependence on the Pt loading.…”
Polymer electrolyte fuel cells (PEFCs) are a promising replacement for the fossil fuel–dependent automotive and energy sectors. They have become increasingly commercialized in the last decade; however, significant limitations on durability and performance limit their commercial uptake. Catalyst layer (CL) design is commonly reported to impact device power density and durability; although, a consensus is rarely reached due to differences in testing conditions, experimental design, and types of data reported. This is further exacerbated by aspects of CL design such as catalyst support, proton conduction, catalyst, fabrication, and morphology, being significantly interdependent; hence, a wider appreciation is required in order to optimize performance, improve durability, and reduce costs. Here, the cutting‐edge research within the field of PEFCs is reviewed, investigating the effect of different manufacturing techniques, electrolyte distribution, support materials, surface chemistries, and total porosity on power density and durability. These are critically appraised from an applied perspective to inform the most relevant and promising pathways to make and test commercially viable cells. This holistic view of the competing aspects of CL design and preparation will facilitate the development of optimized CLs, especially the incorporation of novel catalyst support materials.
“…We reported that the PtSn alloy was inserted in the heterointerface between Pt and SnO 2 , and then, the Pt catalyst became well-orientated along with the relaxation of the lattice distortion and formation of the intermediate phase of PtSn alloy. The latter would diminish the effect of a possible Schottky barrier, enhance the high electronic conductivity, and impede the movement of Pt catalyst particles, as reported in previous papers. − , The loading amounts of Pt 100– x Co x alloy were 15.4 wt % ( x = 19), 16.4 wt % ( x = 23), 18.6 wt % ( x = 24-HR), 17.4 wt % ( x = 25), and 17.9 wt % ( x = 33). The chemical composition ratios (Pt/Co) of all of the catalysts also corresponded well to the chemical ratios measured by ICP-MS.…”
Section: Resultsmentioning
confidence: 61%
“…The Pt 75 Co 25 alloy was also well-oriented with respect to the Ta–SnO 2 support (inset of Figure ). In our previous paper, we evaluated the interface between the Pt catalyst and the SnO 2 support by XPS, hard X-ray photoelectron spectroscopy (HAXPES), and STEM–EDX and confirmed that the PtSn metal alloy layer was inserted at the interface . The PtSn metal alloy was formed during the heat treatment procedure after the Pt catalyst was deposited on the SnO 2 support.…”
Section: Resultsmentioning
confidence: 81%
“…In our previous paper, we evaluated the interface between the Pt catalyst and the SnO 2 support by XPS, hard X-ray photoelectron spectroscopy (HAXPES), and STEM−EDX and confirmed that the PtSn metal alloy layer was inserted at the interface. 50 The PtSn metal alloy was formed during the heat treatment procedure after the Pt catalyst was deposited on the SnO 2 support. We reported that the PtSn alloy was inserted in the heterointerface between Pt and SnO 2 , and then, the Pt catalyst became wellorientated along with the relaxation of the lattice distortion and formation of the intermediate phase of PtSn alloy.…”
We
succeeded in the synthesis of two types of PtCo alloy catalysts supported
on Ta-doped SnO2 without using carbon black additives.
The PtCo disordered alloy supported on Ta–SnO2 (BET
surface area, 37 m2 g–1) with a unique
fused-aggregate network microstructure was confirmed to show 3 times
higher oxygen reduction reaction activity compared to that of a commercial
Pt catalyst supported on carbon black (TEC10E50E, Tanaka Kikinzoku
Co.) from the results of rotating disk electrode (RDE) measurements.
PtCo alloy catalysts supported on Ta-doped SnO2 (PtCo/Ta–SnO2) that were heat-treated under reducing conditions for longer
times formed a Pt-rich phase on the surface of the alloy catalyst.
These PtCo/Ta–SnO2 catalysts with a Pt-rich surface
phase exhibited more than 4 times higher kinetically controlled current
density for the oxygen reduction reaction as well as a higher load
cycle durability, in comparison with those of a commercial PtCo alloy
catalyst supported on graphitized carbon black. PtCo/Ta–SnO2 catalysts with a Pt-rich surface phase are attractive candidates
for polymer electrolyte fuel cell cathodes for fuel cell vehicles.
“…From these observations, a pronounced core–shell structure with an Er-rich shell is indicated for sample A, whereas in sample B, intermixing between Y, Yb, and Er with a slight enrichment of Yb in the near-surface region is consistent with the data. Such spatial distribution of the sensitizer and activator ions enables control of the donor–acceptor interaction and dynamics thereby eliminating or reducing deleterious cross-relaxation between lanthanide dopants and thus fine tuning of the optical properties [ 68 , 69 ]. Additionally, the location of emitting Er 3+ centres in the shell region enables very efficient luminescence resonance energy transfer (LRET) to organic molecules bound to the surface of the UCNPs due to the minimum distance between LRET donors and acceptors.…”
Section: The Ideal Case—a First Look On Oleic Acid Stabilized Yber-do...mentioning
Core–shell nanoparticles have attracted much attention in recent years due to their unique properties and their increasing importance in many technological and consumer products. However, the chemistry of nanoparticles is still rarely investigated in comparison to their size and morphology. In this review, the possibilities, limits, and challenges of X-ray photoelectron spectroscopy (XPS) for obtaining more insights into the composition, thickness, and homogeneity of nanoparticle coatings are discussed with four examples: CdSe/CdS quantum dots with a thick coating and a small core; NaYF4-based upconverting nanoparticles with a large Yb-doped core and a thin Er-doped coating; and two types of polymer nanoparticles with a poly(tetrafluoroethylene) core with either a poly(methyl methacrylate) or polystyrene coating. Different approaches for calculating the thickness of the coating are presented, like a simple numerical modelling or a more complex simulation of the photoelectron peaks. Additionally, modelling of the XPS background for the investigation of coating is discussed. Furthermore, the new possibilities to measure with varying excitation energies or with hard-energy X-ray sources (hard-energy X-ray photoelectron spectroscopy) are described. A discussion about the sources of uncertainty for the determination of the thickness of the coating completes this review.
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