Abstract:The e g ↑ / ͑t 2g ↓ + e g ↓͒ band ratio in cation-substituted La-Fe oxides is identified in O ͑1s͒ x-ray absorption spectra as a linear spectral indicator for conducting electron holes. The t 2g ↓ and e g ↓ bands act as a conductivity inhibitor by ferromagnetic double exchange coupling on the e g ↑ electron. Disorder induced by substitution appears to modulate the hole conduction such that an exponential relation is found between the conductivity and the e g ↑ / ͑t 2g ↓ + e g ↓͒ ratio and hole concentration. T… Show more
“…represent the unoccupied oxygen 2p orbitals and also reflect the empty Fe/Ni 3d bands at the pre-edge (524 eV -527 eV). The triplet at around 525 eV can be attributed to bands of e g (↑), t 2g (↓) and e g (↓) bands [21]. Comparing the pre-edge region of the spectra shown in Figure 6, we can easily identify that the intensity of e g (↑) peak increases with increasing Sr content in the samples.…”
The conductivity of the electron hole and polaron conductor La 1-x , which forms conducting electron holes. Here we have in addition a B-site substitution by Ni. The compound for x = 0.5 is identified as the one with the highest conductivity (σ ~ 678 S/cm) and lowest activation energy for polaron conductivity (E p = 39 meV). The evolution of the electronic structure was monitored by soft x-ray Fe and oxygen K-edge spectroscopy. Homogeneous trend for the oxidation state of the Fe was observed. The variation of the ambient temperature conductivity and activation energy with relative Sr content (x) shows a correlation with the ratio of (e g /e g +t 2g ) in Fe L3 edge up to x=0.5. The hole doping process is reflected by an almost linear trend by the variation of the prepeaks of the oxygen K-edge soft x-ray absorption spectra.2
“…represent the unoccupied oxygen 2p orbitals and also reflect the empty Fe/Ni 3d bands at the pre-edge (524 eV -527 eV). The triplet at around 525 eV can be attributed to bands of e g (↑), t 2g (↓) and e g (↓) bands [21]. Comparing the pre-edge region of the spectra shown in Figure 6, we can easily identify that the intensity of e g (↑) peak increases with increasing Sr content in the samples.…”
The conductivity of the electron hole and polaron conductor La 1-x , which forms conducting electron holes. Here we have in addition a B-site substitution by Ni. The compound for x = 0.5 is identified as the one with the highest conductivity (σ ~ 678 S/cm) and lowest activation energy for polaron conductivity (E p = 39 meV). The evolution of the electronic structure was monitored by soft x-ray Fe and oxygen K-edge spectroscopy. Homogeneous trend for the oxidation state of the Fe was observed. The variation of the ambient temperature conductivity and activation energy with relative Sr content (x) shows a correlation with the ratio of (e g /e g +t 2g ) in Fe L3 edge up to x=0.5. The hole doping process is reflected by an almost linear trend by the variation of the prepeaks of the oxygen K-edge soft x-ray absorption spectra.2
“…We begin this discussion with an example from solid oxide fuel cell cathodes, which are typically built from metal oxides with ABO 3 Experimental spectroscopic evidence is then provided in the oxygen K-shell X-ray absorption spectra, which are recorded with X-ray energy of around 520-560 eV. Whereas the LaFeO 3 with Fe 3+ has in the pre-edge a nice e g -t 2g doublet, the substituted compound with a portion of Fe 4+ shows an additional peak in the NEXAFS spectra, representative of the electron hole, L. It has been shown that the relative spectral weight of this hole peak scales exponentially with the electronic conductivity of the compound [60,61].…”
Section: Characterization Of Metal Oxidesmentioning
In situ and operando techniques can play important roles in the development of better performing photoelectrodes, photocatalysts, and electrocatalysts by helping to elucidate crucial intermediates and mechanistic steps. The development of high throughput screening methods has also accelerated the evaluation of relevant photoelectrochemical and electrochemical properties for new solar fuel materials. In this chapter, several in situ and high throughput characterization tools are discussed in detail along with their impact on our understanding of solar fuel materials.
“…High temperature oxidation and reduction studies [34] and catalysis studies [36] have also been made recently with in-situ or operando sulphur XAS, for example. Sulphur as the ligand ion is also of interest in connection with metal ions [37] and could in future studies open up new opportunities for the understanding and quantification of electronic transport processes in SOFC anodes, where newly formed NieS compounds are subject to exchange interactions, in analogy to 3d metal oxides at SOFC cathodes, for example [38,39]. Latter would constitute an extension of sulphur XAS from molecular structure and chemical speciation of sulphur motifs towards electronic structure, valence band and electronic transport properties of aged SOFC anodes.…”
h i g h l i g h t s g r a p h i c a l a b s t r a c tAn operando SOFC anode S-poisoning XAS experiment at 550 C to 250 C was performed. S K-edge XANES spectral information at Ni/GDC outer surface was collected.Intermediates with different sulphur oxidation states (6þ, 4þ, 0, 2À) were observed. Proportion of oxidation states changed as a function of temperature. Differences between TD calculations and XAS information were observed and discussed. a r t i c l e i n f o a b s t r a c t Sulphur poisoning of nickelebased solid oxide fuel cell (SOFC) anode catalysts is a well-documented shortcoming, but not yet fully understood. Here, a novel experiment is demonstrated to obtain spectroscopic information at operando conditions, in particular the molecular structure of sulphur species in the sulphur K-shell X-ray absorption near edge structure (XANES) region for a SOFC anode under realistic operando conditions, thus, with the flux of O 2À from cathode to anode. Cooling from T ¼ 550 C stepwise down to 250 C, 5 ppm H 2 S/H 2 reacting with Ni-gadolinium doped ceria (GDC) anode resulted in several sulphur species in different oxidation states (6þ, 4þ, 0, À2) and in amounts being at a minimum at high temperature. According to sulphur speciation analysis, the species could either relate to eSO 4 2À or SO 3 (g), eSO 3 2À or SO 2 (g), S 2 (g) or surface-adsorbed S atoms, and, Ni or Ce sulphides, respectively. The coexistence of different sulphur oxidation states as a function of temperature was analysed in the context of thermodynamic equilibrium calculations. Deviations between experimental results and calculations are most likely due to limitations in the speed of some intermediate oxidation steps as well as due to differences between stoichiometric CeO 2 used in calculations and partially reduced Ce 0.9 Gd 0.1 O 2Àd .
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