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Micro-texture measurement in
SEM-EBSD
Principle of Pattern formation in EBSD
For EBSD, a beam of electrons is directed at a point of
interest on a tilted crystalline sample in SEM
The following steps need to be followed to get the
Kikuchi pattern:
• Tilt the specimen to get optimum backscattered
efficiency
• Stop the scanning of surface in SEM to make
stationary electron beam
• Placement of a recording medium to record the
diffracted backscattered electron in SEM
Schematic of an SEM-EBSD set up
Tilting of sample in SEM for EBSD: It is Critical
It reduces the path length of backscattered electrons
escaping from sample after diffraction thus enhance the
data resolution
• The electron/sample interaction volume modifies from
pear shape to shallow depth volume
• The beam circular sizes starts distorting to elliptical with
the tilting of the sample thus reduces the resolution
• Incident beam size : Tilting Increase  Bad resolution
Optimum = 70o to the horizontal (Experimental
optimization of efficiency and resolution
• Because the diffraction pattern is bound to the crystal
structure of the sample, as the crystal orientation
changes the resultant diffraction pattern also
changes
• Intersections of the Kikuchi bands
correspond to the intersection of
zone axes in the crystal. These
points can be labeled by the
crystal direction for the zone axis
where, l is the distance from the sample to the
screen. Hence, planes with wide d-spacings give
thinner Kikuchi bands than narrow planes
• The width w of the Kikuchi bands close to the pattern
center is given by
w  2l  (nl/d)
• Therefore, positions of the Kikuchi bands can be used
to calculate the orientation of the diffracting crystal
Interpretation of EBSD pattern
 The centre lines of the Kikuchi
bands correspond to the
projection of the diffracting
planes on the phosphor screen.
 Each Kikuchi band can be
indexed by Miller indices of the
diffracting crystal plane which
formed it.
 Each point on the phosphor
screen corresponds to the
intersection of a crystal
direction with the screen.
Diffracting crystal
planes (hkl)
Bragg angle
Trace of the (hkl)
plane projected onto
the screen
Electron
Diffracted electrons
(hkl) Kikuchi band
2θ
Representation of Kikuchi patterns (one stereographic
triangle)
FCC BCC
• Crystal orientation is calculated from the Kikuchi band
positions by the computer processing the digitized
diffraction pattern collected by the CCD camera.
Automated indexing and orientation measurement
 = x cos θ + y sin θ
• The Kikuchi band positions
are found using the Hough
transform. The transform
between the coordinates (x,y)
of the diffraction pattern and
the coordinates (ρ, θ) of
Hough space is given by
• A straight line is characterized by
(i) the perpendicular distance from the origin (ρ) and (ii)
the angle made with the x-axis (θ)
• Therefore a line is represented by a single point (ρ, θ) in
Hough space. Kikuchi bands transform to bright regions
in Hough space which can be detected and used to
calculate the original positions of bands.
• Using the system calibration, the angles between the
planes producing the detected Kikuchi bands can be
calculated.
• These are compared with a list of inter-planar angles for
the analyzed crystal structure to allocate Miller indices to
each plane.
1. What should be the experimental precautions should be taken
during EBSD?
2. Explain the tilting of sample in EBSD experiment.
3. What is Hough space?
4. Explain the orientation determination from Kikuchi pattern.
5. How does capturing angle affect in identifying microstructure
constituents?
Question

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l.pdf

  • 2. Principle of Pattern formation in EBSD For EBSD, a beam of electrons is directed at a point of interest on a tilted crystalline sample in SEM The following steps need to be followed to get the Kikuchi pattern: • Tilt the specimen to get optimum backscattered efficiency • Stop the scanning of surface in SEM to make stationary electron beam • Placement of a recording medium to record the diffracted backscattered electron in SEM
  • 3. Schematic of an SEM-EBSD set up
  • 4. Tilting of sample in SEM for EBSD: It is Critical It reduces the path length of backscattered electrons escaping from sample after diffraction thus enhance the data resolution
  • 5. • The electron/sample interaction volume modifies from pear shape to shallow depth volume • The beam circular sizes starts distorting to elliptical with the tilting of the sample thus reduces the resolution • Incident beam size : Tilting Increase  Bad resolution Optimum = 70o to the horizontal (Experimental optimization of efficiency and resolution
  • 6. • Because the diffraction pattern is bound to the crystal structure of the sample, as the crystal orientation changes the resultant diffraction pattern also changes
  • 7. • Intersections of the Kikuchi bands correspond to the intersection of zone axes in the crystal. These points can be labeled by the crystal direction for the zone axis where, l is the distance from the sample to the screen. Hence, planes with wide d-spacings give thinner Kikuchi bands than narrow planes • The width w of the Kikuchi bands close to the pattern center is given by w  2l  (nl/d) • Therefore, positions of the Kikuchi bands can be used to calculate the orientation of the diffracting crystal
  • 8. Interpretation of EBSD pattern  The centre lines of the Kikuchi bands correspond to the projection of the diffracting planes on the phosphor screen.  Each Kikuchi band can be indexed by Miller indices of the diffracting crystal plane which formed it.  Each point on the phosphor screen corresponds to the intersection of a crystal direction with the screen. Diffracting crystal planes (hkl) Bragg angle Trace of the (hkl) plane projected onto the screen Electron Diffracted electrons (hkl) Kikuchi band 2θ
  • 9. Representation of Kikuchi patterns (one stereographic triangle) FCC BCC
  • 10. • Crystal orientation is calculated from the Kikuchi band positions by the computer processing the digitized diffraction pattern collected by the CCD camera. Automated indexing and orientation measurement  = x cos θ + y sin θ • The Kikuchi band positions are found using the Hough transform. The transform between the coordinates (x,y) of the diffraction pattern and the coordinates (ρ, θ) of Hough space is given by
  • 11. • A straight line is characterized by (i) the perpendicular distance from the origin (ρ) and (ii) the angle made with the x-axis (θ) • Therefore a line is represented by a single point (ρ, θ) in Hough space. Kikuchi bands transform to bright regions in Hough space which can be detected and used to calculate the original positions of bands.
  • 12. • Using the system calibration, the angles between the planes producing the detected Kikuchi bands can be calculated. • These are compared with a list of inter-planar angles for the analyzed crystal structure to allocate Miller indices to each plane.
  • 13. 1. What should be the experimental precautions should be taken during EBSD? 2. Explain the tilting of sample in EBSD experiment. 3. What is Hough space? 4. Explain the orientation determination from Kikuchi pattern. 5. How does capturing angle affect in identifying microstructure constituents? Question