In solid-state physics, the concept of Brillouin zones is crucial for understanding the behavior of electrons in a crystal lattice. The Brillouin zone is defined as the set of points in reciprocal space that are closer to a given lattice point than to any other.
For an FCC (Face-Centered Cubic) lattice, the first Brillouin zone is obtained by constructing the Wigner-Seitz cell in reciprocal space. The Wigner-Seitz cell is essentially the region of space that is closer to a given lattice point than to any other. For FCC lattices, this shape takes the form of a truncated octahedron.
A truncated octahedron has 6 square faces, 8 hexagonal faces, and 12 edges. It can be thought of as an octahedron (a polyhedron with 8 triangular faces) where the corners have been truncated, resulting in the formation of square faces. This geometry is a key feature of the first Brillouin zone for FCC crystals.
Therefore, the correct shape of the first Brillouin zone of an FCC lattice is a truncated octahedron.