Abstract

We have performed core level photoelectron spectroscopy on a W(110) single crystal with femtosecond XUV pulses from the free-electron laser at Hamburg (FLASH). We demonstrate experimentally and through theoretical modelling that for a suitable range of photon fluences per pulse, time-resolved photoemission experiments on solid surfaces are possible. Using FLASH pulses in combination with a synchronized optical laser, we have performed femtosecond time-resolved core-level photoelectron spectroscopy and observed sideband formation on the W 4f lines indicating a cross correlation between femtosecond optical and XUV pulses.

Highlights

  • Generation at optical lasers, even femtosecond dynamics have been investigated [35]

  • Our objective is to find suitable x-ray fluences per pulse for electron spectroscopy and derive a generally valid model based on the photon energy dependent photoionization crosssection and the target density

  • The statistics of the spectra vary due to the differences in the number of pulses accumulated with the respective number of photons per pulse, as displayed in the right-hand panel of figure 1, with the latter reflecting the probability distribution of pulse energies of free-electron laser at Hamburg (FLASH) resulting from the self amplified spontaneous emission (SASE) process

Read more

Summary

Introduction

Generation at optical lasers, even femtosecond dynamics have been investigated [35]. there we are restrained to some few wavelengths available from the high harmonics of the laser. If we want to use x-ray pulses for time resolved ESCA in a broad wavelength regime and up to high energies, we need to resort to free-electron lasers (FELs) capable of producing brilliant x-ray pulses up to kilo-electron-volt photon energies with less than 30 fs pulse duration. In this contribution, we establish the foundation for femtosecond time-resolved ESCA (fs-ESCA) on a solid surface using the free-electron laser at Hamburg (FLASH) [36] in combination with a synchronized optical laser. On the sample an optical excitation intensity of 4.62 × 1010 W cm−2 was reached

Objectives
Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call