convergent-beam electron diffraction

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PASI Santiago, Chile July 2006 1 es / Convergent-Beam Diffraction: II Convergent-beam electron diffraction Applications

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Convergent-beam electron diffraction. Applications. Bragg’s Law. Applications - in common with spot patterns. 1Lattice spacings 2Unit cell 3Orientation. Applications - special to CBED Established. 1Crystal symmetry 2Local strain 3Direct phase identification 4Thickness. - PowerPoint PPT Presentation

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Page 1: Convergent-beam electron diffraction

PASI Santiago, Chile July 20061Eades / Convergent-Beam Diffraction: II

Convergent-beam electron diffraction

Applications

Page 2: Convergent-beam electron diffraction

PASI Santiago, Chile July 20062Eades / Convergent-Beam Diffraction: II

Bragg’s Law

sin2d

Page 3: Convergent-beam electron diffraction

PASI Santiago, Chile July 20063Eades / Convergent-Beam Diffraction: II

Applications - in common with spot patterns

• 1 Lattice spacings

• 2 Unit cell

• 3 Orientation

Page 4: Convergent-beam electron diffraction

PASI Santiago, Chile July 20064Eades / Convergent-Beam Diffraction: II

Applications - special to CBEDEstablished

• 1 Crystal symmetry

• 2 Local strain

• 3 Direct phase identification

• 4 Thickness

Page 5: Convergent-beam electron diffraction

PASI Santiago, Chile July 20065Eades / Convergent-Beam Diffraction: II

Applications - special to CBEDAdvanced

• 1 Crystal structure determination

• 2 Bonding measurement

• 3 Phase determination

• 4 Improved defect analysis

Page 6: Convergent-beam electron diffraction

PASI Santiago, Chile July 20066Eades / Convergent-Beam Diffraction: II

Advanced Techniques

• The Tanaka methods– The techniques

• LACBED

• Other variations (CBIM, SA-CBED)

– Applications• Spatial variation

• Defect analysis

• Other Techniques– Coherent CBED– Energy filtering

Page 7: Convergent-beam electron diffraction

PASI Santiago, Chile July 20067Eades / Convergent-Beam Diffraction: II

Lattice Spacings

The lattice spacing is determined from the distance between the diffracted beams.

In spot patterns it is the distance between spots. In convergent-beam patterns it is the distance between discs.

These are generally equally accurate.

Page 8: Convergent-beam electron diffraction

PASI Santiago, Chile July 20068Eades / Convergent-Beam Diffraction: II

FeS2 [110] K-C Hsieh

Page 9: Convergent-beam electron diffraction

PASI Santiago, Chile July 20069Eades / Convergent-Beam Diffraction: II

Unit Cell Determination

If a very short camera length is used, the unit cell can be determined, in principle, from a single diffraction pattern.

In practice this may be tricky.

The centering of the Bravais lattice can be easily obtained at a suitable zone axis.

Page 10: Convergent-beam electron diffraction

PASI Santiago, Chile July 200610Eades / Convergent-Beam Diffraction: II

Page 11: Convergent-beam electron diffraction

PASI Santiago, Chile July 200611Eades / Convergent-Beam Diffraction: II

Orientation

If the diffraction pattern is indexed, the orientation of the sample is determined.

A selected area pattern can determine the orientation to within a few degrees.

In convergent-beam diffraction additional information, from details in the discs or from Kikuchi lines, gives the result to a fraction of a degree.

Page 12: Convergent-beam electron diffraction

PASI Santiago, Chile July 200612Eades / Convergent-Beam Diffraction: II

Symmetry

The determination of the symmetry of a crystalline specimen is one of the most powerful applications of convergent-beam diffraction. It is valuable both to identify known phases and to determine the symmetry of new phases.

Page 13: Convergent-beam electron diffraction

PASI Santiago, Chile July 200613Eades / Convergent-Beam Diffraction: II

Page 14: Convergent-beam electron diffraction

PASI Santiago, Chile July 200614Eades / Convergent-Beam Diffraction: II

Pyrite [001] K-C Hsieh

Page 15: Convergent-beam electron diffraction

PASI Santiago, Chile July 200615Eades / Convergent-Beam Diffraction: II

Strain from HOLZ lines

• Limitations– The strain must be uniform through the

thickness of the specimen.– The result is for the strain in the thin foil - not

the strain in the original sample.– Results are relative not absolute without

dynamical calculation.

Page 16: Convergent-beam electron diffraction

PASI Santiago, Chile July 200616Eades / Convergent-Beam Diffraction: II

Page 17: Convergent-beam electron diffraction

PASI Santiago, Chile July 200617Eades / Convergent-Beam Diffraction: II

Page 18: Convergent-beam electron diffraction

PASI Santiago, Chile July 200618Eades / Convergent-Beam Diffraction: II

Page 19: Convergent-beam electron diffraction

PASI Santiago, Chile July 200619Eades / Convergent-Beam Diffraction: II

Page 20: Convergent-beam electron diffraction

PASI Santiago, Chile July 200620Eades / Convergent-Beam Diffraction: II

Page 21: Convergent-beam electron diffraction

PASI Santiago, Chile July 200621Eades / Convergent-Beam Diffraction: II

Page 22: Convergent-beam electron diffraction

PASI Santiago, Chile July 200622Eades / Convergent-Beam Diffraction: II

Page 23: Convergent-beam electron diffraction

PASI Santiago, Chile July 200623Eades / Convergent-Beam Diffraction: II

Phase Identification

• All convergent-beam zone axis patterns are unique and serve to identify phases.

• You must educate your eye.

• Limitations– The patterns do change with thickness– The uniqueness is not absolute.

Page 24: Convergent-beam electron diffraction

PASI Santiago, Chile July 200624Eades / Convergent-Beam Diffraction: II

V3Si Doug Konitzer

Page 25: Convergent-beam electron diffraction

PASI Santiago, Chile July 200625Eades / Convergent-Beam Diffraction: II

InP [100] G. Rackham

Page 26: Convergent-beam electron diffraction

PASI Santiago, Chile July 200626Eades / Convergent-Beam Diffraction: II

M23C6 [110]

Page 27: Convergent-beam electron diffraction

PASI Santiago, Chile July 200627Eades / Convergent-Beam Diffraction: II

Ni3Al [110] S. Court

Page 28: Convergent-beam electron diffraction

PASI Santiago, Chile July 200628Eades / Convergent-Beam Diffraction: II

Ni3Al [110] S. Court

Page 29: Convergent-beam electron diffraction

PASI Santiago, Chile July 200629Eades / Convergent-Beam Diffraction: II

Thickness

• The method uses two-beam conditions.

• Some care must be taken in the analysis.

• The thickness is for the crystalline part of the sample only.

Page 30: Convergent-beam electron diffraction

PASI Santiago, Chile July 200630Eades / Convergent-Beam Diffraction: II

Page 31: Convergent-beam electron diffraction

PASI Santiago, Chile July 200631Eades / Convergent-Beam Diffraction: II

Page 32: Convergent-beam electron diffraction

PASI Santiago, Chile July 200632Eades / Convergent-Beam Diffraction: II

Page 33: Convergent-beam electron diffraction

PASI Santiago, Chile July 200633Eades / Convergent-Beam Diffraction: II

Crystal Structure

• The phase problem

• Crystal structure determination

• Bonding measurement

Page 34: Convergent-beam electron diffraction

PASI Santiago, Chile July 200634Eades / Convergent-Beam Diffraction: II

Crystal Potential

)2exp()( rg g.gr iVV

Page 35: Convergent-beam electron diffraction

PASI Santiago, Chile July 200635Eades / Convergent-Beam Diffraction: II

• Because of the complex interference between diffracted beams in dynamical electron diffraction, electron diffraction intensities are very sensitive to small changes in Vg.

• Electron diffraction can thus determine bonding electron densities - but the calculations are complicated.

Page 36: Convergent-beam electron diffraction

PASI Santiago, Chile July 200636Eades / Convergent-Beam Diffraction: II

Midgley, Saunders, Vincent and Steeds Ultramicroscopy 59 (1995) 1-13

Page 37: Convergent-beam electron diffraction

PASI Santiago, Chile July 200637Eades / Convergent-Beam Diffraction: II

Midgley, Saunders, Vincent and Steeds Ultramicroscopy 59 (1995) 1-13

Page 38: Convergent-beam electron diffraction

PASI Santiago, Chile July 200638Eades / Convergent-Beam Diffraction: II

Tanaka, Terauchi, Tsuda and Saitoh CBED IV 2002

Page 39: Convergent-beam electron diffraction

PASI Santiago, Chile July 200639Eades / Convergent-Beam Diffraction: II

Tanaka, Terauchi and Tsuda CBED III 1994

Page 40: Convergent-beam electron diffraction

PASI Santiago, Chile July 200640Eades / Convergent-Beam Diffraction: II

The Tanaka Methods

• Traditional microscopy taught that the microscope should be focussed on the specimen or on the diffraction pattern in the back focal plane.

• Tanaka liberated us and gave rise to a family of new techniques by telling us to look in other places.

Page 41: Convergent-beam electron diffraction

PASI Santiago, Chile July 200641Eades / Convergent-Beam Diffraction: II

S p ec im e n S p ec im e n S p ec im e n

Page 42: Convergent-beam electron diffraction

PASI Santiago, Chile July 200642Eades / Convergent-Beam Diffraction: II

GaAs [100] K. Christenson

Page 43: Convergent-beam electron diffraction

PASI Santiago, Chile July 200643Eades / Convergent-Beam Diffraction: II

Ni3Mo

Page 44: Convergent-beam electron diffraction

PASI Santiago, Chile July 200644Eades / Convergent-Beam Diffraction: II

Ni3Mo BF Tanaka pattern

Page 45: Convergent-beam electron diffraction

PASI Santiago, Chile July 200645Eades / Convergent-Beam Diffraction: II

Al layer on GaAs Tanaka Group

Page 46: Convergent-beam electron diffraction

PASI Santiago, Chile July 200646Eades / Convergent-Beam Diffraction: II

Defect Analysis

• Large-Angle Convergent-Beam patterns provide an improved method of determining the Burgers vectors of dislocations. (And characterizing other defects.)

• The dislocations have to be well separated.

Page 47: Convergent-beam electron diffraction

PASI Santiago, Chile July 200647Eades / Convergent-Beam Diffraction: II

Fe,30Ni,19Cr [114] Cherns and Preston

Page 48: Convergent-beam electron diffraction

PASI Santiago, Chile July 200648Eades / Convergent-Beam Diffraction: II

Fe,30Ni,19Cr [114] Cherns and Preston

Page 49: Convergent-beam electron diffraction

PASI Santiago, Chile July 200649Eades / Convergent-Beam Diffraction: II

Fe,30Ni,19Cr [114] Cherns and Preston

Page 50: Convergent-beam electron diffraction

PASI Santiago, Chile July 200650Eades / Convergent-Beam Diffraction: II

Si Tanaka Group

Page 51: Convergent-beam electron diffraction

PASI Santiago, Chile July 200651Eades / Convergent-Beam Diffraction: II

• My apologies to those whose pictures are not acknowledged because I do not remember where they came from.

• All the Ni3Mo pictures are Mike Kaufman’s work.