Zero-energy photoelectric effect

Fuente: arXiv
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Autori principali: Azizi, Sajad, Saalmann, Ulf, Rost, Jan M.
Natura: Preprint
Pubblicazione: 2024
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author Azizi, Sajad
Saalmann, Ulf
Rost, Jan M.
author_facet Azizi, Sajad
Saalmann, Ulf
Rost, Jan M.
contents We predict a near-threshold ("zero energy") peak in multi-photon ionization for a dynamical regime where the photon frequency is large compared to the binding energy of the electron. The peak position does not depend on the laser frequency, but on the binding energy and the pulse duration. The effect originates from the fact that bound-continuum dipole transitions are stronger than continuum-continuum ones. To clearly observe this zero-energy photoelectric effect, the spectral width of the laser pulse should be comparable to the binding energy of the ionized orbital, and the second ionization potential should be larger than the photon energy. This suggests negative ions as ideal candidates for corresponding experiments.
format Preprint
id arxiv_https___arxiv_org_abs_2407_16270
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Zero-energy photoelectric effect
Azizi, Sajad
Saalmann, Ulf
Rost, Jan M.
Atomic Physics
We predict a near-threshold ("zero energy") peak in multi-photon ionization for a dynamical regime where the photon frequency is large compared to the binding energy of the electron. The peak position does not depend on the laser frequency, but on the binding energy and the pulse duration. The effect originates from the fact that bound-continuum dipole transitions are stronger than continuum-continuum ones. To clearly observe this zero-energy photoelectric effect, the spectral width of the laser pulse should be comparable to the binding energy of the ionized orbital, and the second ionization potential should be larger than the photon energy. This suggests negative ions as ideal candidates for corresponding experiments.
title Zero-energy photoelectric effect
topic Atomic Physics
url https://arxiv.org/abs/2407.16270