1. Suppression of the vacuum space-charge effect in fs-photoemission by a retarding electrostatic front lens.
- Author
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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., and Manschwetus, B.
- Subjects
HARD X-rays ,FREE electron lasers ,PHOTOELECTRONS ,ELECTROSTATIC fields ,PHOTOEMISSION ,MAGNITUDE (Mathematics) ,STORAGE rings ,SPACE charge - 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 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 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. [ABSTRACT FROM AUTHOR]- Published
- 2021
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