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Suppression of the vacuum space-charge effect in fs-photoemission by a retarding electrostatic front lens

Authors :
Siarhei Dziarzhytski
Steffen Palutke
Michael Heber
Kai Rossnagel
Thomas K. Allison
Katerina Medjanik
S. Babenkov
Yu. Matveyev
Laurenz Rettig
V. Shokeen
Bastian Manschwetus
Ingmar Hartl
S. K. Mahatha
D. Vasilyev
Nora Schirmel
Martin Beye
Gerd Schönhense
Frederico Pressacco
Harald Redlin
Steinn Ymir Agustsson
G. Brenner
O. Fedchenko
B. Schönhense
Hans-Joachim Elmers
Lukas Wenthaus
D. Kutnyakhov
Andrei Gloskovskii
N. Wind
H. Duerr
Christoph Schlueter
S. Chernov
Source :
Review of Scientific Instruments, Review of scientific instruments 92(5), 053703 (2021). doi:10.1063/5.0046567
Publication Year :
2021
Publisher :
Deutsches Elektronen-Synchrotron, DESY, Hamburg, 2021.

Abstract

Review of scientific instruments 92(5), 053703 (2021). doi:10.1063/5.0046567<br />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 E$_{kin}$ = 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 E$_{kin}$ = 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 E$_{kin}$ = 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/cm$^2$ (retarding field −21 V/mm). For an accelerating field of +2 kV/mm and a pump fluence of only 5 mJ/cm$^2$, 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 E$_{kin}$ = 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.<br />Published by American Institute of Physics, [S.l.]

Details

Language :
English
Database :
OpenAIRE
Journal :
Review of Scientific Instruments, Review of scientific instruments 92(5), 053703 (2021). doi:10.1063/5.0046567
Accession number :
edsair.doi.dedup.....fcc1b5023d34507aeec1e96b9b27b011
Full Text :
https://doi.org/10.3204/pubdb-2021-03880