Anandh Subramaniam & Kantesh Balani

Slides:



Advertisements
Similar presentations
Don’t Ever Give Up!.
Advertisements

Sai Nandyala.  Determination of crystal structure internally  Every lattice plane behaves like a diffraction grating when X-rayed  Position of spectral.
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
4. Investigations into the electrical properties of particular metals at different temperatures led to the identification of superconductivity and the.
XRD Line Broadening With effects on Selected Area Diffraction (SAD) Patterns in a TEM MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani.
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Weak Interactions Non-Covalent Interactions MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE)
(0,0) RECIPROCAL LATTICE (0,1) (1,1) (2,1) (3,1) REAL LATTICE a b a* b*
Anandh Subramaniam & Kantesh Balani
EEE539 Solid State Electronics
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Gratings. Double Slit Resolution  The bright bands from a double slit are wide. Exact maximum difficult to determine  There is a broad area with some.
 In these set of slides we will try to visualize how constructive and destructive interference take place (using the Bragg’s view of diffraction as ‘reflection’
Miller Indices And X-ray diffraction
Analysis of crystal structure x-rays, neutrons and electrons
KINETICS MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur-
Anandh Subramaniam & Kantesh Balani
DISLOCATION STRESS FIELDS  Dislocation stress fields → infinite body  Dislocation stress fields → finite body  Image forces  Interaction between dislocations.
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Anandh Subramaniam & Kantesh Balani
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
FATIGUE Fatigue of Materials (Cambridge Solid State Science Series) S. Suresh Cambridge University Press, Cambridge (1998) MATERIALS SCIENCE &ENGINEERING.
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Anandh Subramaniam & Kantesh Balani
Graphene MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur-
Anandh Subramaniam & Kantesh Balani
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Anandh Subramaniam & Kantesh Balani
Ø. Prytz Introduction to diffraction Øystein Prytz January
SAMPLE XRD PATTERNS MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology,
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Crystal Structure and Crystallography of Materials Chapter 14: Diffraction Lecture No. 2.
CHARACTERIZATION OF THE STRUCTURE OF SOLIDS
If a single slit diffracts, what about a double slit?
Seminar on X-ray Diffraction
Diffraction in TEM Janez Košir
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
1D, 2D, 3D…. nD Euclidian, Spherical, Hyperbolic General Riemannian
The theory of diffraction
Chem E5225 – Electron Microscopy P
de Broglie Waves de Broglie argued
General Physics (PHY 2140) Lecture 28 Modern Physics Quantum Physics
MATERIALS SCIENCE &ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
X Ray Diffraction © D Hoult 2009.
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
X-Rays.
X-Ray Diffraction and Reciprocal Lattice
Anandh Subramaniam & Kantesh Balani
If a single slit diffracts, what about a double slit?
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Electron Diffraction Experiment
Analysis of crystal structure x-rays, neutrons and electrons
Today’s agenda: Thin Film Interference.
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Bragg Diffraction 2dsinq = nl Bragg Equation
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Anandh Subramaniam & Kantesh Balani
Body centered cubic Note that each corner atom is in eight cubes so only 1/8 of the corner atom is in this cell Number of atoms = 1 center + 8 x 1/8 corners.
X-Ray Diffraction Path Length Phase Difference
Presentation transcript:

Anandh Subramaniam & Kantesh Balani Looking at Bragg’s equation a few tantalizing questions come to our mind:  There is no mention of interatomic spacing in the plane!  What about in-plane scattering wherein incident  scattered  but the waves are still in phase We take up these questions in this set of slides MATERIALS SCIENCE & ENGINEERING Anandh Subramaniam & Kantesh Balani Materials Science and Engineering (MSE) Indian Institute of Technology, Kanpur- 208016 Email: anandh@iitk.ac.in, URL: home.iitk.ac.in/~anandh AN INTRODUCTORY E-BOOK Part of http://home.iitk.ac.in/~anandh/E-book.htm A Learner’s Guide

Note that in the Bragg’s equation: The interatomic spacing (a) along the plane does not appear Only the interplanar spacing (d) appears  Change in position or spacing of atoms along the plane should not affect Bragg’s condition !! d Note: shift (systematic) is actually not a problem!

Note: shift is actually not a problem Note: shift is actually not a problem!  Why is ‘systematic’ shift not a problem?

Consider the case for which 1  2 Constructive interference can still occur if the difference in the path length traversed by R1 and R2 before and after scattering are an integral multiple of the wavelength  (AY − XC) = h  (h is an integer)

This is looking at diffraction from atomic arrays and not planes Generalizing into 3D Laue’s equations S0  incoming X-ray beam S  Scattered X-ray beam This is looking at diffraction from atomic arrays and not planes

A physical picture of scattering leading to diffraction is embodied in Laue’s equations Bragg’s method of visualizing diffraction as “reflection” from a set of planes is a different way of understanding the phenomenon of diffraction from crystals The ‘plane picture’ (Bragg’s equations) are simpler and we usually stick to them Hence, we should think twice before asking the question: “if there are no atoms in the scattering planes (actually a subset of the planes being considered), how are they scattering waves?”