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Direct Energy, 2018a

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120 6.4 Crystallography Revisited<br />

Lattice vectors in real space have units of length, m. Lattice vectors in<br />

reciprocal space have units m −1 .<br />

The reciprocal lattice gives information about the spatial frequency of<br />

atoms. If the planes of atoms in a crystal are closely spaced in one direction,<br />

| −→ a 1 | is relatively small. The corresponding reciprocal vector | −→ b 1 | is relatively<br />

large. The reciprocal lattice represents the spatial frequency of the atom<br />

in units m −1 . If the planes of atoms in a crystal are far apart, | −→ a 1 | is large<br />

and | −→ b 1 | is small.<br />

If a beam of light shines on a crystal where the wavelength of light<br />

is close to the crystal spacing, light will be diracted, and the diraction<br />

pattern is related to the reciprocal lattice. The Brillouin zone is a primitive<br />

cell for a reciprocal lattice. The volume of a unit cell in reciprocal space<br />

over a unit cell in real space is given by<br />

vol. Brillouin zone<br />

vol. primitive cell in real space = −→<br />

b1 · −→ b 2 × −→ b 3<br />

−→ a1 · −→ a 2 × −→ a 3<br />

=(2π) 3 . (6.18)<br />

As for the real space lattice, to understand the reciprocal space lattice,<br />

we need to only understand one cell because the reciprocal space lattice is<br />

periodic.<br />

6.4.2 E versus k Diagrams<br />

The energy level diagrams, discussed in Section 6.3, plot allowed energies<br />

of electrons where the vertical axis represented energy. No variation is<br />

shown on the horizontal axis. The most useful energy level diagrams for<br />

semiconductors are zoomed in so that only the valence and conduction<br />

band are shown. In many cases, it is useful to plot energy level diagrams<br />

versus position in real space. For such a diagram the vertical axis represents<br />

energy, and the horizontal axis represents position. It is also useful to plot<br />

energy level diagrams versus position in reciprocal space.<br />

Kinetic energy is given by<br />

E kinetic = 1 2 m|−→ v | 2 = 1<br />

2m |−→ M| 2 (6.19)<br />

where −→ v represents velocity in m s and m represents mass in kg. Momentum<br />

is given by −→ M = m −→ v in units kg·m<br />

s = J·s<br />

m . Electrons in crystals at<br />

T>0 K vibrate, and certain vibrations are resonant in the crystal. The<br />

crystal momentum −→ M crystal represents the internal momentum of due to<br />

vibrations. It can be expressed as<br />

−→<br />

M crystal = −→ k (6.20)

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