Forskjell mellom versjoner av «Diffraction»
Fra Nanowiki
(→Bragg's law) |
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Linje 16: | Linje 16: | ||
*Allowed and forbidden reflections |
*Allowed and forbidden reflections |
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− | In the FCC (face-centered cubic) lattice the Miller indices have to be all odd or all even. |
+ | In the FCC (face-centered cubic) lattice the Miller indices have to be all odd or all even./ |
In the BCC (body-centeres cubic) lattice the sum of h+k+l must be odd for an allowed reflection. |
In the BCC (body-centeres cubic) lattice the sum of h+k+l must be odd for an allowed reflection. |
Revisjonen fra 24. mai 2009 kl. 13:38
Background
Crystalline, polycrystalline and amorphous materials.
The crystal lattice: unit cell and point lattices. The seven crystal systems. Space groups. Miller indices and Unit vectors. Reciprocal space.
Some diffraction properties and conditions
- Elastic scattering (no energy loss).
- The wavelength of the radiation should be comparable to the interatomic spacing of the material.
Bragg's law
- Condition: The planes of atoms responsible for a diffraction peak have to behave as a specula mirror, so that the angle of incidence \theta equals the angle of reflection.
- Bragg's law
- <math> n\lambda=2dsin\theta </math>
where n is an integer, \lambda is the wavelength of the radiation, d is the spacing of the crystal lattice planes and \theta is is the reflection angle.
- Allowed and forbidden reflections
In the FCC (face-centered cubic) lattice the Miller indices have to be all odd or all even./ In the BCC (body-centeres cubic) lattice the sum of h+k+l must be odd for an allowed reflection.