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6.3.1.3 Medium and high energy ion scattering

Chapter Concepts

Properties LEED; RHEED; crystal structure; electron scattering data; ion scattering data; lattice parameter; surface determination; surface structure
Keywords interaction; introduction; surface
Substrates atom; charged particle

Source

Title

6.3.1.3 Medium and high energy ion scattering

In

6.3.1 Introduction

Author P. Alkemade
Part of Landolt-Börnstein - Group III Condensed Matter
Numerical Data and Functional Relationships in Science and Technology
Volume

24c: Interaction of Charged Particles and Atoms with Surfaces

Edited by G. Chiarotti
Chapter-DOI 10.1007/10086066_42
Book-DOI 10.1007/b87125 (Volume in Bookshelf)

Cite as

RIS-Export Alkemade, P.: 6.3.1.3 Medium and high energy ion scattering. Chiarotti, G. (ed.). SpringerMaterials - The Landolt-Börnstein Database (http://www.springermaterials.com). DOI: 10.1007/10086066_42

Abstract

6.3.1.3 Medium and high energy ion scattering in '6.3.1 Introduction', part of 'Landolt-Börnstein - Group III Condensed Matter: Numerical Data and Functional Relationships in Science and Technology, Volume 24c: Interaction of Charged Particles and Atoms with Surfaces'.
This chapter talks about medium and high energy ion scattering (MEIS and HEIS). MEIS and HEIS spectrometry and LEED intensity-voltage (IV) analysis are the two main experimental techniques for surface relaxation determination. LEED reveals long range order and MEIS and HEIS reveal short range order in a surface. Since the penetration depth of the probing ions (usually 0.05 to 3 MeV H+ or He+) is between hundreds of nanometers and several micrometers, MEIS and HEIS as such are not surface analysis techniques. The distinction between MEIS and HEIS is mainly instrumental; the underlying physics is the same and, therefore, treated here together. Remarkable for MEIS/HEIS is the simplicity of the underlying physics. For medium and high energies, neutralization is not excessively high. Moreover, it is independent of the particle’s trajectory. Of course, if a solid state detector is used, both backscattered ions and neutrals are detected without any discrimination. Furthermore, the collisions of the ions in the crystal can be fully regarded as binar; collisions. And, since scattering cross sections are relatively small, almost all detected ions are backscattered in one single hard collision: double and multiple scatterings are rare. The required ion accelerator and beam steering optics are in contrast more complicated and expensive than for LEIS.