Reciprocal Lattice & Diffraction

Slides:



Advertisements
Similar presentations
Objectives By the end of this section you should:
Advertisements

Reciprocal Space Learning outcomes
XII. Electron diffraction in TEM
IX. X-ray diffraction 9-1. Production of X-ray Vacuum, thermionic emission, high voltage,
What is diffraction? Diffraction – the spreading out of waves as they encounter a barrier.
X-Ray Experiment Presenter: Xu Luo Dec 16, Part 1. Introduction  Powder method A monochromatic X-ray beam scatters off the randomly oriented powder.
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
X-Ray Crystallography The most important technique for mineralogy The most important technique for mineralogy Direct measurement of atomic arrangement.
(0,0) RECIPROCAL LATTICE (0,1) (1,1) (2,1) (3,1) REAL LATTICE a b a* b*
Followed by a few examples of
Reciprocal lattice How to construct reciprocal lattice
Announcements 1)Revised Lab timings: 1-3 PM (all groups) 2) Quiz 1, 28 th Jan 2014, Tuesday 7:30 PM, WS 209, WS 213.
Crystallography and Diffraction Techniques Myoglobin.
Reciprocal Space This chapter has been downloaded onto the Mech 580 Electron Microscopy website. Since the reciprocal lattice does not pertain to electron.
Solid State Physics 2. X-ray Diffraction 4/15/2017.
Introduction and point groups Stereographic projections Low symmetry systems Space groups Deformation and texture Interfaces, orientation relationships.
Expression of d-dpacing in lattice parameters
© Oxford Instruments Analytical Limited 2001 MODULE 2 - Introduction to Basic Crystallography Bravais Lattices Crystal system Miller Indices Crystallographic.
Shared by 8 unit cells Shared by 2 unit cells.
SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples
Xray crystallography Lasse Mårtensson, IFM-Chemistry.
TEM- What is it?. Diffraction in the Transmission Electron Microscope Vidhya Sagar Jayaseelan.
X-Ray Diffraction ME 215 Exp#1. X-Ray Diffraction X-rays is a form of electromagnetic radiation having a range of wavelength from nm (0.01x10 -9.
Analysis of crystal structure x-rays, neutrons and electrons
Exercise: Indexing of the electron diffraction patterns
VIII. Kinematical Theory of Diffraction 8-1. Total Scattering Amplitude The path difference between beams scattered from the volume element apart is The.
X-ray Diffraction Outline Crystals and Bragg Diffraction
Analysis of crystal structure x-rays, neutrons and electrons
X-ray Diffraction What are X-rays?  E-M waves : Characterized by high frequency, high energy  Wavelength: 0.01 – 10 nm  Invisible to Human Eye (Visible.
X-ray diffraction. Braggs' law = 2d hkl sin  hkl X-ray diffraction From this set of planes, only get reflection at one angle -  From this set of planes,
XI. Reflection high energy electron diffraction
Page 1 Phys Baski Diffraction Techniques Topic #7: Diffraction Techniques Introductory Material –Wave-like nature of electrons, diffraction/interference.
Overview of Solid State Physics Starting from the Drude Model.
The Braggs and X ray Crystallography By sending radiation through crystal structures you should be able to produce diffraction around the atoms.
Crystallography Lecture notes Many other things.
Sections 12.1 – 12.2 Types of Solids Metallic Solids.
Lecture_08: Outline Matter Waves  de Broglie hypothesis  Experimental verifications  Wave functions.
Crystal Structure and Crystallography of Materials Chapter 14: Diffraction Lecture No. 2.
SHKim 2007 Lecture 4 Reciprocal lattice “Ewald sphere” Sphere of reflection (diffraction) Sphere of resolution.
Sad Analysis Dewsdado gabriel poba baquisse BT/ME/1601/017.
Crystallography H. K. D. H. Bhadeshia Introduction and point groups
© 1997, Angus Rockett Section I Evaporation.
Seminar on X-ray Diffraction
Ch.4 Atomic Structure of Solid Surfaces.
Basic Crystallography
youtube. com/watch. v=WIoS7WJDZT8 youtube
Ewald construction Think of set of planes reflecting in x-ray beam.
Increase the number of visible reflections more information
X-ray diffraction.
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Crystallography H. K. D. H. Bhadeshia Introduction and point groups
Materials Science and Metallurgy Course C6: Crystallography
Crystallography H. K. D. H. Bhadeshia Introduction and point groups
The Electromagnetic Spectrum
Materials Science and Metallurgy Mathematical Crystallography
Crystallography H. K. D. H. Bhadeshia Introduction and point groups
Diffraction T. Ishikawa Part 1 Kinematical Theory 1/11/2019 JASS02.
Crystallography H. K. D. H. Bhadeshia Introduction and point groups
500 nm WRITE VOLTAGE 0 V.
Deformation and texture
Electron Diffraction Experiment
Electron diffraction Øystein Prytz.
Crystallography H. K. D. H. Bhadeshia Introduction and point groups
Group theory for the periodic lattice
Bragg Diffraction 2dsinq = nl Bragg Equation
Counting Atoms in Unit Cells:
Crystal structure determination and space groups
Counting Atoms in Unit Cells:
Chapter 16: Electron Diffraction
Crystallography Orientation relationships Metric tensor
Presentation transcript:

Reciprocal Lattice & Diffraction Crystallography H. K. D. H. Bhadeshia Reciprocal Lattice & Diffraction

Weiss Zone Rule proven!

Cubic P, section of reciprocal lattice normal to [001]

Cubic P, section of reciprocal lattice normal to [110]

Cubic P, section of reciprocal lattice normal to [111]

For 100 keV accelerating voltage, the wavelength of electrons is 0 For 100 keV accelerating voltage, the wavelength of electrons is 0.0037 nm. If the d spacing is 0.2 nm, then the Bragg angle is just 0.5° Ewald sphere has a large diameter in reciprocal space.

Cubic P Cubic F

Cubic P Cubic F

Cubic P Cubic F

Lattice: face-centred cubic Motif: Si at 0,0,0 Si at 1/4,1/4,1/4 3/4 1/4 3/4 1/4 3/4 1/4 3/4 1/4 Lattice: face-centred cubic Motif: Si at 0,0,0 Si at 1/4,1/4,1/4

diffraction from thin crystals

100 nm thick foil 20 nm thick foil

[111] [0.99 0.99 1.02]

(R. Herring)