The control of electron distribution excited in a metal through optical phase of the excitation light is demonstrated. Two-photon photoemission from the Cu(111) surface is excited either by a pair of ~15fs laser pulses with a mutual delay fixed to an accuracy of ±0.025fs, or by a single, frequency-chirped pulse. As a consequence of optical coherence in the two-photon excitation process, the photoemission spectra do not only depend on the frequency, as in conventional spectroscopy, but also on the phase of the excitation light. This may be a general phenomenon in multiphoton ionization.
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Petek et al. (1997) studied this question.
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