Crystal structure

Lattice and basis

Screenshot 2024-09-23 113448.png

📖 Definitions:

🗒️ Note: the main focus will be on $\rm 3D$ lattices

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📖 Definitions:

🗒️ Note: there are many different primitive vectors for one lattice (they all have the same area or volume)

💃 Example: we can re-write the lattice vector as

$$ \vec R=n_1(\vec a_1+ \vec a_2)+ (n_2-n_1) \vec a_2+n_3 \vec a_3 $$

which is a new set of primitive lattice vectors with $\vec a_1 + \vec a_2 ,\vec a_2,\vec a_3$

Bragg Scattering

X-ray scattering from parallel planes

X-ray scattering from parallel planes

Properties:

Unit cells

<aside> <img src="https://prod-files-secure.s3.us-west-2.amazonaws.com/369dfa6b-d4d9-4cf2-a446-e369553b6347/4347c2ad-fb72-4991-bec6-b41f3d2592d1/Primitive_unit_cell.png" alt="https://prod-files-secure.s3.us-west-2.amazonaws.com/369dfa6b-d4d9-4cf2-a446-e369553b6347/4347c2ad-fb72-4991-bec6-b41f3d2592d1/Primitive_unit_cell.png" width="40px" />

Primitive unit cell: Any region of space that contains only one lattice point and can be translated by lattice vectors $\vec R$ to fill the whole space without leaving gaps or forming overlaps

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💃 Example: The parallelepiped whose edges are the primitive vectors $\vec a_1, \vec a_2,\vec a_3$ is always a primitive unit cell.