This spectrum shows that 31P signal is dominated by a broad peak, which can unambiguously be ascribed to solid-state 31P given its short T2 of ~85 μs (FWHM ~18.5 ppm) and long T1 of ~20 s (fitted from spectra acquired for five different TR, data not shown).
Since changes in voltammograms with time of resting of the alloy in an inert atmosphere were found, they were ascribed to solid state reactions of formation of compounds richer in copper from the one richer in cadmium (or pure cadmium) and pure copper.
The first transitions were ascribed to solid-solid transitions resulting from a large increase in disorder of the side chains.
Alternatively, this may be ascribed to substantial areal organization differences.
From the second cycle, the reduction peak shifts from 0.49 to 0.54 V, which could be ascribed to the formation of solid electrolyte interphase (SEI) layer and lithium-driven structural modifications [39 41].
Notably, the first discharge capacities for Ni0.75Co0.25MoO4 and NiMoO4 were higher than their theoretical capacities; this might be ascribed to the formation of the solid electrolyte interface-like organic layer.
Moreover, it may also be ascribed to the hydrolysis of PO43− in solid phase [ 34].
The high turbidity can be ascribed to larger particles, such as dissolved solids and organic matter in the surface water samples (Schafer et al. 2010).
The enhanced light emission in the solid state may be ascribed to the propeller-like dye architectures, which sterically hinder the intermolecular π π interactions rather than the intramolecular charge transfer.
Higher total dissolved solids in thermal water can be ascribed to high-temperature water-rock interaction at great depth.
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