cbed patterns - introduction probe the electron probe can be made on the order of 0.1 nm so very...

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EM C ourse – C B ED Patterns ProfessorR odney H erring

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Page 1: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

EM Course – CBED Patterns

Professor Rodney Herring

Page 2: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED Patterns - Introduction

Page 3: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED Patterns - Introduction

probe

The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled.

Page 4: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED Patterns - Introduction

Perfect for the characterization of nanoparticles

Page 5: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED Patterns - Introduction

Energy-filtered TEM

Page 6: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED vs SAD Patterns

Page 7: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED vs SAD Patterns

A wealth of crystal information

Page 8: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

Making a TEM CBED Pattern

Page 9: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

Making a TEM CBED Pattern

Page 10: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

Making a STEM CBED Pattern

L, camera length

Page 11: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

Making (S)TEM CBED Patterns

If the specimen is uniform, its CBED pattern doesn’t move while the beam is scanned through the specimen.

Page 12: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

Experimental Variables

Page 13: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED Convergence Angle,

Page 14: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED Cameral Length, L

Page 15: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

Beam Diameter, specimen thickness

Page 16: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED Patterns - Focus

DF = Dark Field; BF = Bright Field

Page 17: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED – Kikuchi & HOLZ Lines

Diffraction of elastically scattered electrons at large angles creates the Laue Zone Lines.

Page 18: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED – Kikuchi & HOLZ Lines

Page 19: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED Pattern

Back-focal plane

Defocused probe

Defocus CBED

Change focus of probe either by using objective lens or manually changing the eucentric height

Page 20: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED – ZOLZ, HOLZ lines

Page 21: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED – ZOLZ, HOLZ lines

Page 22: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED – Energy Filtering

Page 23: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED – Energy Filtering

There are many more details concerned with CBED imaging in Williams & Carter, which I don’t have time to present, that I want to review in Chapter 20.

Page 24: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

CBED – Lattice Strain Measurements

d could be the change in interplanar spacing, d, due to strain. It causes the ZOLZ lines and HOLZ lines to split. This type of measurement of strain provides the highest resolution measurement of strain in crystals.

Page 25: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

HOLZ Line Strain Measurement

Beam direction

Page 26: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

HOLZ Line Strain Measurement

Unstrained Strained

Experimental images of strain measurement by HOLZ lines at an interface between Si substrate and Si+Ge epilayer.

Next we will apply electron holography to split HOLZ lines to measure their phase.

Page 27: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

Diffracted Beam Holography of HOLZ Line Strain Measurements

Split HOLZ line is self-interfered by placing an electron biprism between the lines and then applying a voltage.

Page 28: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

Diffracted Beam Holography of HOLZ Line Strain Measurements

Fig 2 – Experimental images showing in a) a split HOLZ line running horizontally through the 000 disc, b) the same split HOLZ line running through a diffraction disc, c) self-interference of the split HOLZ line by the biprism and d) same as c) but increased biprism voltage.

Page 29: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

Diffracted Beam Holography of HOLZ Line Strain Measurements

Higher magnification of Fig 2d showing the fringes more clearly and phase shifts existing at the intersections with other HOLZ lines, for example, at arrow.

Herring et al, “Coherent Electron Interference of a split HOLZ line from a Strained Silicon Crystal” Microscopy & Microanalysis 2011. Submitted.

The current challenge is to measure the 3D strain field from 2D information.

Page 30: CBED Patterns - Introduction probe The electron probe can be made on the order of 0.1 nm so very small volumes can be sampled

K-M – Kossel - MÖllenstedt