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EM C ourse – Elastic Scattering ProfessorR odney H erring
23

Elastic Scattering - Introduction Transverse Waves particles and waves.

Dec 21, 2015

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Page 1: Elastic Scattering - Introduction Transverse Waves particles and waves.

EM Course – Elastic Scattering

Professor Rodney Herring

Page 2: Elastic Scattering - Introduction Transverse Waves particles and waves.

Elastic Scattering - Introduction

Transverse Waves

particles and waves

Page 3: Elastic Scattering - Introduction Transverse Waves particles and waves.

Elastic Scattering of Electrons

Page 4: Elastic Scattering - Introduction Transverse Waves particles and waves.

Elastic Scattering of Electrons

Page 5: Elastic Scattering - Introduction Transverse Waves particles and waves.

1 Point Source 2 Point Sources

Interference

Page 6: Elastic Scattering - Introduction Transverse Waves particles and waves.

Elastic Scattering of Electrons

Page 7: Elastic Scattering - Introduction Transverse Waves particles and waves.

Elastic Scattering of Electrons

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Scattering Cross Section of Electrons

For electrons scattering from the nucleus to high angles, the differential cross-section is given by,

For electrons scattering from the nucleus to high angles, the total nuclear cross-section is given by,

The beam energy, Eo, the angle of scattering and the atomic number, Z, all affect the probability that an electron will be scattered by the nuclei of atoms in the specimen. These expressions cannot calculate the cross sections exactly because they only consider the particle nature of electrons and ignore their wave nature.

Page 9: Elastic Scattering - Introduction Transverse Waves particles and waves.

Scattering Cross Section of Electrons

For C, a 1 MV TEM does very little radiation damage to the specimen!

Page 10: Elastic Scattering - Introduction Transverse Waves particles and waves.

Mean Free Path of Electrons

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Atomic Scattering Factor, fThe Rutherford expressions of electron scattering could not calculate the cross sections exactly because they only considered the particle nature of electrons and ignored their wave nature.A full wave mechanics treatment of scattering cross sections is well beyond the scope of this course.The easiest and most familiar concept used is the atomic-scattering factor, f), which is related to the differential elastic cross section by,

Page 12: Elastic Scattering - Introduction Transverse Waves particles and waves.

Atomic Scattering Factor, f

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0 .2 0 .4 0 .6 0 .8 1 .0

10

20

30

40

50

Zero-loss & Phonon-loss Intensities for Gallium Arsenide (GaAs)

s (1/Å)

0 10 20

(mrad)

222 444 666 atomic planes

Doyle and Turner Acta Cryst. (1968). A24, 390

Intensity

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Atomic Scattering Factor, f

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THE Structure Factor, F

Page 16: Elastic Scattering - Introduction Transverse Waves particles and waves.

THE Structure Factor, F

An example follows

Page 17: Elastic Scattering - Introduction Transverse Waves particles and waves.

THE Structure Factor, F

Page 18: Elastic Scattering - Introduction Transverse Waves particles and waves.

THE Structure Factor, F

Page 19: Elastic Scattering - Introduction Transverse Waves particles and waves.

THE Structure Factor, F

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Diffraction Equations

Page 21: Elastic Scattering - Introduction Transverse Waves particles and waves.

Diffraction Equations

1915

(Sir William H. Bragg and Mr. W. Lawrence Bragg)(father - son team)

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Diffraction Equations• As seen before, the destructive and constructive interference of a

beam of x-rays or electrons off atomic planes is shown below.

Destructive Interference Constructive Interference

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Chapter Summary