“…We note that this shoulder feature can be subtle (and even go unnoticed) when the Ir L IIIedge spectra are collected with standard resolution and is not always reported for Y 2 Ir 2 O 7 or other AIr x O y materials. 6,8,14,24,28,29 To prove this, we collected Ir L III -edge XAS on the same material using a beamline with standard resolution and did not observe the same clear splitting of the peak (Figure S6), consistent with previous reports showing the advantages of HERFD-XAS at the Ir L III -edge. 30 This distinctive peak shape measured by HERFD-XAS is attributed to the different electronic configuration of Ir in Y 2 Ir 2 O 7 , where electron correlations and spin−orbit coupling are known to split the Ir 5d t 2g orbital into e″ and u′ orbitals, 23,24,31,32 whereas all five d valence electrons in IrO 2 occupy the t 2g orbital that spans the Fermi level, the d electrons in Y 2 Ir 2 O 7 fill the u′ orbital and half-fill the higher energy e″ orbital with localized empty states above the Fermi level.…”