Abstract

Velocity map imaging (VMI) spectrometry is widely used to measure the momentum distribution of charged particles with the kinetic energy of a few tens of electronVolts. With the progress of femtosecond laser and X-ray free-electron laser, it becomes increasingly important to extend the electron kinetic energy to 1 keV. Here, we report on a recently built composite VMI spectrometer at the Shanghai soft X-ray free-electron laser, which can measure ion images and high-energy electron images simultaneously. In the SIMION simulation, we extended the electron kinetic energy to 1 keV with a resolution <2% while measuring the ions with the kinetic energy of 20 eV. The experimental performance is tested by measuring Ar 2p photoelectron spectra at Shanghai Synchrotron Radiation Facility, and O+ kinetic energy spectrum from dissociative ionization of O2 by 800 nm femtosecond laser. We reached a resolution of 1.5% at the electron kinetic energy of 500 eV. When the electron arm is set for 100 eV, a resolution of 4% is reached at the ion kinetic energy of 5.6 eV. This composite VMI spectrometer will support the experiment, such as X-ray multi-photon excitation/ionization, Auger electrons emission, attosecond streaking.

Highlights

  • Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations

  • The standard velocity map imaging (VMI) spectrometer was originally designed by Eppink and Parker in 1997 [1], which consists of a repeller, an open extractor, and a flight tube

  • We reached a resolution of 1.5% at the electron kinetic energy of 500 eV, and the

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Summary

Introduction

The velocity map imaging (VMI) spectrometer is a powerful tool to obtain a highresolution projected two-dimensional (2D) image of the three-dimensional (3D) momentum distribution of charged particles, which was widely used in atomic and molecular physics. The standard VMI spectrometer was originally designed by Eppink and Parker in 1997 [1], which consists of a repeller, an open extractor, and a flight tube. The charged particles are created at the crossing region where the light beam meets the molecular beam. They are driven towards a two-dimensional position-sensitive detector. With the well-designed electric field, the radius that the charged particle impact on the detector depends only on its initial radial momentum and is almost independent of the source position

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