A.E. GunnsMENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope.

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A.E. Gunnæs MENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope

description

A.E. GunnæsMENA3100 V08 Basic TEM Electron source (HV= 200kV) Apertures Sample holder Fluorescence screen Film box Pedals for tilting the sample Magnetic lenses Vacuum in the column better than Pa

Transcript of A.E. GunnsMENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope.

Page 1: A.E. GunnsMENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope.

A.E. Gunnæs MENA3100 V08

Electron Diffraction (ED) in the transmissions electron microscope

Page 2: A.E. GunnsMENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope.

A.E. Gunnæs MENA3100 V08

JEOL 2010F in the Research park

Page 3: A.E. GunnsMENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope.

A.E. Gunnæs MENA3100 V08

Basic TEMElectron source (HV= 200kV)

Apertures

Sample holder

Fluorescence screen

Film box

Pedals for tilting the sample

Magnetic lenses

Vacuum in the columnbetter than 10-6 Pa

Page 4: A.E. GunnsMENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope.

A.E. Gunnæs MENA3100 V08

The lenses and apertures in a TEM

Sample

Filament

Anode

ΔU= ~100-1000 kV

1. and 2. condenser lenses

Objective lens

Intermediate lenses

Projector lens

Selected area aperture(diffraction aperture)

Objective aperture

Condenser aperture

Electron source:

●Tungsten, W

● LaB6

● FEG

ImageFluorescence Screen (ZnS or ZnS/CdS powder)

Recording media:

●Film

● Imaging plates

● CCD camera

●TV camera

λ= h/(2meV)0.5

(NB non rel. Expr)

Page 5: A.E. GunnsMENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope.

A.E. Gunnæs MENA3100 V08

Simplified ray diagram

Objective lense

Diffraction plane(back focal plane)

Image plane

Sample

Parallel incoming electron beamSi

a

b

cPow

derCell 2.0

1,1 nm

3,8

Å

Convergent beam -Discs in diffraction -Micro diffraction -STEM mode -Chemical analysis

Page 6: A.E. GunnsMENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope.

A.E. Gunnæs MENA3100 V08

Electron diffraction

Elastic scattered electronsOnly the direction of v is changing.(Bragg scattering)

Elastic scattering is due to Coulomb interaction between the incident electrons and the electric charge of the electron clouds and the nucleus. (Rutherford scattering).

The elastic scattering is due to the average position of the atoms in the lattice.

Reflections satisfying Braggs law:

2dsinθ=nλ

Inelastic scattered electronsDirection and magnitude of v change.

Energy is transferred to electrons and atoms in the sample.

-It is due to the movements of the atoms around their average position in the lattice.

- It give rise to a diffuse background in the diffraction patterns.

Electrons interacts 100-1000 times stronger with matter than X-rays-more absorption (need thin samples)-can detect weak reflections not observed with x-rays

Page 7: A.E. GunnsMENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope.

A.E. Gunnæs MENA3100 V08

Sample preparationTEM grids

3 mm

Page 8: A.E. GunnsMENA3100 V08 Electron Diffraction (ED) in the transmissions electron microscope.

A.E. Gunnæs MENA3100 V08

Sample holders

Sample positions

Cooling

Standard

Heating