Abstract

Using a spectrally resolved electron interferometry technique, we measure photoionization time delays between the $3s$ and $3p$ subshells of argon over a large 34-eV energy range covering the Cooper minima in both subshells. The observed strong variations of the $3s-3p$ delay difference, including a sign change, are well reproduced by theoretical calculations using the Two-Photon Two-Color Random Phase Approximation with Exchange. Strong shake-up channels lead to photoelectrons spectrally overlapping with those emitted from the $3s$ subshell. These channels need to be included in our analysis to reproduce the experimental data. Our measurements provide a stringent test for multielectronic theoretical models aiming at an accurate description of inter-channel correlation.

Highlights

  • Half a century after their theoretical description by Eisenbud [1], Wigner [2], and Smith [3], scattering delays— called Wigner delays—can be measured using attosecond spectroscopy, which allows for detailed studies of the correlated interactions within various quantum systems

  • 3s subshell, interorbital correlation is important, since the 3p → εd process is strongly coupled to 3s → ε p [35]. This leads to a correlation-induced “replica” of the 3p Cooper minima (CM) in the 3s ionization channel, close to 42-eV photon energy, as shown in Fig. 1 [36]. All these correlation effects are expected to leave an imprint on the scattering and photoionization delays between the 3s and 3p electrons, which motivated a large number of calculations during the past decade in the demanding region above the 3s threshold [11,12,37,38,39,40,41,42,43,44,45]

  • The methods qualitatively agree on the behavior of the 3p atomic delays, which are slightly negative over a large energy region around the 3p CM

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Summary

Introduction

Half a century after their theoretical description by Eisenbud [1], Wigner [2], and Smith [3], scattering delays— called Wigner delays—can be measured using attosecond spectroscopy, which allows for detailed studies of the correlated interactions within various quantum systems. This leads to a correlation-induced “replica” of the 3p CM in the 3s ionization channel, close to 42-eV photon energy, as shown in Fig. 1 [36].

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