Fig. 3

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Optical responses of AgxIn1-x (left) and AgxAl1-x (right) for x = 0.75 (light blue), x = 0.50 (green) and x = 0.25 (deep purple). (c, d): experimental spectra of BNPs embedded in silica. AgxAl1-x BNPs were size-selected, while AgxIn1-x BNPs were not. For both compositions, the higher the proportion of Al or In, the more the resonance is blue-shifted. (a, b) simulations performed within the multi-shell model structure. The dotted lines correspond to absorption spectra of AgXoIn1-Xo@In and AgXoAl1-Xo@Al BNPs for the three nominal proportions of silver x = 0.25, 0.50 and 0.75, with Xo = 0.75. In such configurations, the LSPRs are always blue-shifted compared to the experimental spectra. The full lines correspond to absorption spectra taking into account the oxidation of the indium or aluminium shell, resulting in multi-shell structures AgXcIn1-Xc@In@In2O3 or AgXcAl1-Xc@Al@Al2O3 where Xc (≠ Xo) is the silver atomic proportion in the core. For Ag-In and for the nominal proportions of silver x = 0.25, 0.50 and 0.75, the values of Xc are 90%, 92.5% and 95% and the volume percentages of indium oxidation Vox are 30%, 50% and 85%, respectively. For Ag-Al, the spectra in full line correspond to silver atomic proportions in the core Xc = 90%, 92.5% and 100% and volume percentages of aluminium oxidation Vox = 97.5%, 100% and 95%, for nominal concentrations x = 0.25, 0.50 and 0.75, respectively. These amounts of In2O3 and Al2O3 were adjusted to obtain the best agreement of the spectral position of the resonance with experimental spectra.
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