Index
Thickness Measurement

All the CBED patterns have been calculated using many-beams dynamical electron diffraction theory (Blochwave approach). They are shown to give worked examples of using this technique for measuring specimen thickness. Example 7 shows how to measure both thickness and CBED defocus. It might be not possible to reproduce experimentally due to the large coherence required to realize it. Furthermore, only calculations based on large artificial super-cells are able to reproduce the fringes observed when the probe size is smaller than the unit-cell size.

Examples
  1. Al, 2-beams dynamical situation.

  2. Si, 2-beams dynamical situation.

  3. Si, [111] axial.

  4. BeO, [120] axial, many beams.

  5. ZnTe, [001] axial, many beams.

  6. Ge, [031], (400) at Bragg condition, many beams.

  7. CaCO3, [110], (003) at Bragg condition, 100kV, many beams.

  8. Si, [011], systematic row, (11-1) at Bragg condition, many beams

  9. GaN [001] axial, many beams.


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Example 1

Al [031], (200) at Bragg condition. Note the large anomalous absorption effect.

Figure1

Figure 1 Al [031], intensity profile.

Figure2

Figure 2 Al [031] many beams fit.


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Example 2

Si [021], (400) near Bragg condition.

Figure3

Figure 3 Si [021] near Bragg condition.

Figure4

Figure 4 Si [021] intensity profile (note the large number of fine details).

Figure5

Figure 5 Si [021] many beams fit.


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Example 3

Si [111], axial, many beams.

Figure6

Figure 6 Si [111].

Figure7

Figure 7 Si [111], intensity profile.

Figure8

Figure 8 Si [111], many beams fit.


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Example 4

BeO [120], axial, many beams, 10 nm thick, incoherent illumination.

Figure9

Figure 9 BeO [120], note the overlapping disks (incoherent illumination).

Figure10

Figure 10 BeO [120], intensity profile, the colored sections show in blue the transmitted disk and in red the diffracted disks. The program creates a data structure that contains information about the overlapping disks.

Figure11

Figure 11 BeO [120] many beams fit. For overlapping disks sections the intensity of the related reflections are added (under coherent illumination condition). The best fit is obtained for 10 nm thick BeO crystal.


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Example 5

ZnTe [001] axial, typical thickness under high resolution conditions.

Figure12

Figure 12 ZnTe [001] axial.

Figure13

Figure 13 ZnTe [001]. 3 nm thick, intensity profile.

Figure14

Figure 14< ZnTe [001] many beams fit.


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Example 6

Ge [031], Bragg condition for (400).

Figure15

Figure 15 Ge [031], (400) at Bragg condition.

Figure16

Figure 16 Ge [031], intensity profile.

Figure17

Figure 17 Ge [031] many beams fit.


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Example 7

CaCO3, [110], (003) at Bragg condition, 100kV.

Figure18

Figure 18 CaCO3 [110], (003) at Bragg condition.

Figure19

Figure 19 CaCO3 [110], intensity profile.

Figure20

Figure 20 CaCO3 many beams fit.


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Example 8

This example shows overlapping Si [011], (000) and (11-1) disks under coherent illumination. The fringes system depends on the probe defocus (above the specimen).

Figure21

Figure 21 (000) and (11-1) CBED disks.

Figure22

Figure 22 Si, intensity profile across coherent disks.

Figure23

Figure 23 Si, many beams fit.


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Example 9

GaN [001] axial, many beams.

Figure24

Figure 24 GaN [001].

Figure25

Figure 25 GaN [001], intensity profile.

Figure26

Figure 26 GaN [001] many beams fit.