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Suppression of the vacuum space-charge effect in fs-photoemission by a retarding electrostatic front lens.
Schönhense, G; Kutnyakhov, D; Pressacco, F; Heber, M; Wind, N; Agustsson, S Y; Babenkov, S; Vasilyev, D; Fedchenko, O; Chernov, S; Rettig, L; Schönhense, B; Wenthaus, L; Brenner, G; Dziarzhytski, S; Palutke, S; Mahatha, S K; Schirmel, N; Redlin, H; Manschwetus, B; Hartl, I; Matveyev, Yu; Gloskovskii, A; Schlueter, C; Shokeen, V; Duerr, H; Allison, T K; Beye, M; Rossnagel, K; Elmers, H J; Medjanik, K.
Afiliação
  • Schönhense G; Johannes Gutenberg-Universität, Institut für Physik, D-55099 Mainz, Germany.
  • Kutnyakhov D; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Pressacco F; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Heber M; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Wind N; University of Hamburg, Institut für Experimentalphysik, D-22761 Hamburg, Germany.
  • Agustsson SY; Johannes Gutenberg-Universität, Institut für Physik, D-55099 Mainz, Germany.
  • Babenkov S; Johannes Gutenberg-Universität, Institut für Physik, D-55099 Mainz, Germany.
  • Vasilyev D; Johannes Gutenberg-Universität, Institut für Physik, D-55099 Mainz, Germany.
  • Fedchenko O; Johannes Gutenberg-Universität, Institut für Physik, D-55099 Mainz, Germany.
  • Chernov S; Departments of Chemistry and Physics, Stony Brook University, Stony Brook, New York 11790-3400, USA.
  • Rettig L; Fritz-Haber-Institut der Max-Planck-Gesellschaft, D-14195 Berlin, Germany.
  • Schönhense B; Department of Bioengineering, Imperial College London, South Kensington Campus, London SW7 2AZ, United Kingdom.
  • Wenthaus L; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Brenner G; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Dziarzhytski S; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Palutke S; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Mahatha SK; Ruprecht Haensel Laboratory, Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Schirmel N; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Redlin H; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Manschwetus B; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Hartl I; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Matveyev Y; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Gloskovskii A; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Schlueter C; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Shokeen V; Department of Physics and Astronomy, Uppsala University, P.O. Box 516, 75120 Uppsala, Sweden.
  • Duerr H; Department of Physics and Astronomy, Uppsala University, P.O. Box 516, 75120 Uppsala, Sweden.
  • Allison TK; Departments of Chemistry and Physics, Stony Brook University, Stony Brook, New York 11790-3400, USA.
  • Beye M; Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Rossnagel K; Ruprecht Haensel Laboratory, Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany.
  • Elmers HJ; Johannes Gutenberg-Universität, Institut für Physik, D-55099 Mainz, Germany.
  • Medjanik K; Johannes Gutenberg-Universität, Institut für Physik, D-55099 Mainz, Germany.
Rev Sci Instrum ; 92(5): 053703, 2021 May 01.
Article em En | MEDLINE | ID: mdl-34243258
ABSTRACT
The performance of time-resolved photoemission experiments at fs-pulsed photon sources is ultimately limited by the e-e Coulomb interaction, downgrading energy and momentum resolution. Here, we present an approach to effectively suppress space-charge artifacts in momentum microscopes and photoemission microscopes. A retarding electrostatic field generated by a special objective lens repels slow electrons, retaining the k-image of the fast photoelectrons. The suppression of space-charge effects scales with the ratio of the photoelectron velocities of fast and slow electrons. Fields in the range from -20 to -1100 V/mm for Ekin = 100 eV to 4 keV direct secondaries and pump-induced slow electrons back to the sample surface. Ray tracing simulations reveal that this happens within the first 40 to 3 µm above the sample surface for Ekin = 100 eV to 4 keV. An optimized front-lens design allows switching between the conventional accelerating and the new retarding mode. Time-resolved experiments at Ekin = 107 eV using fs extreme ultraviolet probe pulses from the free-electron laser FLASH reveal that the width of the Fermi edge increases by just 30 meV at an incident pump fluence of 22 mJ/cm2 (retarding field -21 V/mm). For an accelerating field of +2 kV/mm and a pump fluence of only 5 mJ/cm2, it increases by 0.5 eV (pump wavelength 1030 nm). At the given conditions, the suppression mode permits increasing the slow-electron yield by three to four orders of magnitude. The feasibility of the method at high energies is demonstrated without a pump beam at Ekin = 3830 eV using hard x rays from the storage ring PETRA III. The approach opens up a previously inaccessible regime of pump fluences for photoemission experiments.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Rev Sci Instrum Ano de publicação: 2021 Tipo de documento: Article País de afiliação: Alemanha

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Rev Sci Instrum Ano de publicação: 2021 Tipo de documento: Article País de afiliação: Alemanha