1 / 15

2. Wave Diffraction and Reciprocal Lattice

2. Wave Diffraction and Reciprocal Lattice. Diffraction of Waves by Crystals Scattered Wave Amplitude Brillouin Zones Fourier Analysis of the Basis Quasicrystals. Diffraction Of Waves By Crystals. Bragg’s Law. Reflectance of each plane is about 10 3 to 10 5. Monochromator.

karsen
Download Presentation

2. Wave Diffraction and Reciprocal Lattice

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. 2. Wave Diffraction and Reciprocal Lattice • Diffraction of Waves by Crystals • Scattered Wave Amplitude • Brillouin Zones • Fourier Analysis of the Basis • Quasicrystals

  2. Diffraction Of Waves By Crystals Bragg’s Law Reflectance of each plane is about 103 to 105 .

  3. Monochromator 1.16A neutron beam on CaF2 Relative intensities are due to basis. X-ray Diffractometer on Powdered Si

  4. Scattered Wave Amplitude Fourier Analysis → where  T → Define then mi integers bi is called the primitive vectors of the reciprocal lattice, and G a reciprocal lattice vector. i,j,k cyclic

  5. Diffraction Conditions Scattering vector Difference in phases between waves scattered at r and O Scattering amplitude 

  6. Diffraction condition: (G  G)   From Problem 1: where  Diffraction condition can be written as Bragg’s law

  7. Laue Equations Diffraction condition: →  k lies in the intersection of 3 cones about the crystal axes. Ewald construction • White dots are reciprocal lattice points. • Incident k drawn with end at lattice point. • Scattered k obtained by drawing a circle.

  8. Brillouin Zones Brillouin Zone  Wigner-Seitz cell of reciprocal lattice. Diffraction condition → → k is on boundary of BZ. Square lattice

  9. Reciprocal Lattice to SC Lattice Primitive lattice vectors: Primitive cell volume: Primitive reciprocal lattice vectors: Reciprocal lattice is also SC.

  10. Reciprocal Lattice to BCC Lattice Primitive lattice vectors: Primitive cell volume: Primitive reciprocal lattice vectors: Reciprocal lattice is FCC. Reciprocal lattice vector: Cartesian coord 1st BZ rhombic dodecahedron bcc

  11. Reciprocal Lattice to FCC Lattice Primitive lattice vectors: Primitive cell volume: Primitive reciprocal lattice vectors: Reciprocal lattice is BCC. Reciprocal lattice vector: Cartesian coord 1st BZ fcc

  12. Fourier Analysis of the Basis Scattering amplitude Structure factor For a basis with s atoms  atomic form factor

  13. Structure Factor of BCC Lattice With respect to the SC lattice, the BCC has a basis of 2 atoms at and → E.g., metallic Na: no (100), (300), (111), or (221) lines (cancelled by extra plane at half separation)

  14. Structure Factor of FCC Lattice With respect to the SC lattice, the FCC has a basis of 4 atoms at →

  15. Atomic Form Factor For a spherical distribution of electron density For For forward scattering, G 0 , so that f  Z. For X-ray diffraction, f Z. ( X-ray not sensitive to change in n(r) caused by bonding)

More Related