Abstract

Scanning transmission electron microscopy (STEM) and scanning electron microscopy (SEM) are prominent techniques for the structural characterization of materials. STEM in particular provides high spatial resolution down to the sub-angstrom range. The spatial resolution in STEM and SEM is ultimately limited by the electron-beam diameter provided by the microscope's electron optical system. However, the resolution is frequently degraded by the interaction between electron and matter leading to beam broadening, which depends on the thickness of the analyzed sample. Numerous models are available to calculate beam broadening. However, most of them neglect the energy loss of the electrons and large-angle scattering. These restrictions severely limit the applicability of the approaches for large sample thicknesses in STEM and SEM. In this work, we address beam broadening in a more general way. We numerically solve the electron transport equation without any simplifications, and take into account energy loss along the electron path. For this purpose, we developed the software package CeTE (Computation of electron Transport Equation). We determine beam broadening, energy deposition, and the interaction volume of the scattered electrons in homogeneous matter. The calculated spatial and angular distributions of electrons are not limited to forward scattering and small sample thicknesses. We focus on low electron energies of 30 keV and below, where beam broadening is particularly pronounced. These electron energies are typical for SEM and STEM in scanning electron microscopes.

Highlights

  • Scanning electron microscopy (SEM) and scanning transmission electron microscopy (STEM) are prominent techniques to study the structural properties of solids and soft matter materials

  • The numerical calculations were performed similar to the approach of Negreanu et al [30], but in this work we have taken into account energy loss by the continuous-slowing-down approximation [27]

  • The results are not limited to electrons energies between 10 and 30 keV, which are typical for scanning electron microscopes, but apply to higher electron energies used in transmission electron microscopes as long as the contribution of coherence effects can be neglected

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Summary

Introduction

Scanning electron microscopy (SEM) and scanning transmission electron microscopy (STEM) are prominent techniques to study the structural properties of solids and soft matter materials. The spatial resolution of images and analytical techniques in electron microscopy does depend on the beam diameter provided by the microscope’s condenser-lens system but is strongly affected by the broadening of the electron beam while passing through matter. This is relevant if the primary electron energy in transmission electron microscopes is lowered from standard values between 80 and 300 keV.

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