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Generalization of the duration-time concept for interpreting high-resolution resonant photoemission spectra

  • R. Feifel
  • , A. Baev
  • , F. Gel’mukhanov
  • , H. Ågren
  • , M. N. Piancastelli
  • , M. Andersson
  • , G. Öhrwall
  • , C. Miron
  • , M. Meyer
  • , S. L. Sorensen
  • , A. Naves de Brito
  • , O. Björneholm
  • , L. Karlsson
  • , S. Svensson
  • Uppsala University
  • KTH Royal Institute of Technology
  • Institute of Automation and Electrometry of the Siberian Branch of the Russian Academy of Sciences
  • University of Rome Tor Vergata
  • Université Paris-Saclay
  • CNRS
  • Lund University
  • Centro Nacional de Pesquisa em Energia e Materiais

Research output: Contribution to journalArticlepeer-review

4 Scopus citations

Abstract

The duration-time concept, vastly successful for interpreting the frequency dependence of resonant radiative and nonradiative x-ray scattering spectra, is tested for fine-scale features that can be obtained with state of the art high-resolution spectroscopy. For that purpose resonant photoelectron (RPE) spectra of the first three outermost singly ionized valence states [Formula Presented] [Formula Presented] and [Formula Presented] are measured for selective excitations to different vibrational levels (up to [Formula Presented] of the N [Formula Presented] photoabsorption resonance in [Formula Presented] and for negative photon frequency detuning relative to the adiabatic 0-0 transition of this resonance. It is found that different parts of the RPE spectrum converge to the spectral profile of direct photoionization (fast scattering) for different detunings, and that the RPE profiles are asymmetrical as a function of frequency detuning. The observed asymmetry contradicts the picture based on the simplified notation of a common scattering duration time, but is shown to agree with the here elaborated concept of partial and mean duration times. Results of the measurements and the simulations show that the duration time of the scattering process varies for different final electronic and different final vibrational states. This owes to two physical reasons: one is the competition between the fast “vertical” and the slow “resonant” scattering channels and the other is the slowing down of the scattering process near the zeros of the real part of the scattering amplitude. 5555 2004 The American Physical Society.

Original languageEnglish
Pages (from-to)12
Number of pages1
JournalPhysical Review A - Atomic, Molecular, and Optical Physics
Volume69
Issue number2
DOIs
StatePublished - 2004

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