Randomized trial measures electron energy distributions in alkali metals, indicating surface-plasmon excitation effects.
Measured energy distributions of photoemitted electrons from K, Rb, and Cs show a high-energy peak identified as unscattered (primary) electrons, and an intermediate peak at somewhat lower energies which is believed to be due to a plasmon energy loss. This intermediate structure becomes more pronounced and closer to the primary peak on proceeding from K to Rb to Cs. This systematic trend, together with the absence of any clearly discernible intermediate structure in Na, is consistent with the variation of the corresponding plasmon energies. In Rb and Cs the intermediate peak is sufficiently pronounced to permit its identification as a surface rather than a volume-plasmon excitation.
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Smith et al. (1969) studied this question.