2018
DOI: 10.1021/acs.inorgchem.8b01219
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Revisiting the Dependence of Cu K-Edge X-ray Absorption Spectra on Oxidation State and Coordination Environment

Abstract: X-ray absorption spectroscopy (XAS) at the Cu K-edge is an important tool for probing the properties of copper centers in transition-metal chemistry and catalysis. However, the interpretation of experimental XAS spectra requires a detailed understanding of the dependence of spectroscopic features on the local geometric and electronic structure, which can be established by theoretical X-ray spectroscopy. Here, we present a systematic computational study of the Cu K-edge XAS spectra of selected Cu complexes base… Show more

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Cited by 40 publications
(61 citation statements)
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“…36,37 The change in the oxidation state of the copper atom, from Cu + into Cu 2+ , leads to the observed 3.3eV shift of the edge energy position, as confirmed by experimental 38 and theoretical studies. 39 The Extended X-ray absorption Fine Structure (EXAFS) spectraextracted via the standard background removal procedure -are shown in Figure 5 b). The XANES and EXAFS spectra versus the annealing temperature are identical for both Cu2O and Cu2O:Mg thin films, except the 450 °C annealing step.…”
Section: Figure 4 Cu 2p Xps Spectra Obtained For the Undoped And Mg-doped Cu2o Thin Films Deposited On Glass Both As-deposited And Annealmentioning
confidence: 99%
“…36,37 The change in the oxidation state of the copper atom, from Cu + into Cu 2+ , leads to the observed 3.3eV shift of the edge energy position, as confirmed by experimental 38 and theoretical studies. 39 The Extended X-ray absorption Fine Structure (EXAFS) spectraextracted via the standard background removal procedure -are shown in Figure 5 b). The XANES and EXAFS spectra versus the annealing temperature are identical for both Cu2O and Cu2O:Mg thin films, except the 450 °C annealing step.…”
Section: Figure 4 Cu 2p Xps Spectra Obtained For the Undoped And Mg-doped Cu2o Thin Films Deposited On Glass Both As-deposited And Annealmentioning
confidence: 99%
“…As mentioned in the Introduction section, one of the motivations for our work was the knowledge that the oxidation state of +1 had been typically observed for Cu in various selenides. Nevertheless, the Cu K -edge spectra of both A-samples and B-samples exhibit a weak pre-edge feature at 8979.5 eV (Figure ), which can be assigned only to the dipole-forbidden 1s → 3d transition of the Cu 2+ ion with the single hole in the 3d orbitals . This assignment is also supported by the fact that the XANES spectrum of Cu 2 Se does not show such a pre-edge feature, with the absorption edge appearing at a notably higher energy, 8982 eV .…”
Section: Resultsmentioning
confidence: 83%
“…50 Similar rising edge shakedown features are observed for Cu(II) complexes which supports our assignment of a (DHP 2−• )Cu(II) electronic structure, however we note that rising edge features are also observed for Cu(I) complexes which convolutes this assignment. [52][53][54][55] The energy of the 1s → 4p transition for 1 is lower than that for square planar Cu(II) complexes, which may reflect that the open coordination site trans to the pyrrole for this T-shaped complex stabilizes the 4px orbital and shifts the transition to lower energy. [56][57][58][59][60] Related rising edge features have also been associated with some Tshaped Cu(I) complexes, where the electric dipole-allowed 1s → 4p transition corresponds to a sharp rising edge peak, although such peaks are typically of a larger normalized intensity than what is observed for 1.…”
Section: Synthesis and Electronic Structure Of 1 Andmentioning
confidence: 99%