Reciprocal Lattice: From Real Space to Diffraction Space

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a* = 2.09 Å⁻¹ — reciprocal lattice

A square real lattice with a = b = 3 Å produces a square reciprocal lattice with a* = b* = 2.09 Å⁻¹ and the Ewald sphere of radius 2 Å⁻¹.

Formula

a* = 2π / (a·sin(γ)), b* = 2π / (b·sin(γ))
γ* = 180° - γ
Diffraction condition: Δk = G (reciprocal lattice vector)

The Dual of Real Space

The reciprocal lattice is one of the most powerful abstractions in physics. For every real-space crystal lattice, there exists a dual lattice in momentum space (reciprocal space) whose points correspond one-to-one with families of crystal planes. This duality transforms the complex geometry of wave scattering into elegant point-matching conditions that underpin all of modern diffraction science.

Construction and Properties

To build the reciprocal lattice, take each real-space lattice vector and construct its reciprocal counterpart: perpendicular to the other two real-space vectors, with magnitude inversely proportional to the real-space spacing. The result is a lattice where large real-space dimensions produce small reciprocal spacings, and vice versa. An oblique real cell with angle γ yields a reciprocal cell with angle 180° - γ.

The Ewald Sphere

The Ewald sphere construction provides an intuitive geometric picture of diffraction. Draw a sphere in reciprocal space with radius 1/λ centered on the crystal. Any reciprocal lattice point touching the sphere surface satisfies the Laue diffraction condition — equivalent to Bragg's law. Rotating the crystal rotates the reciprocal lattice, sweeping different points through the sphere and producing different diffraction spots.

Beyond Diffraction

Reciprocal space extends far beyond X-ray crystallography. Brillouin zones — primitive cells of the reciprocal lattice — define the natural domain for electronic band theory and phonon dispersion. Fermi surfaces live in reciprocal space. Fourier transforms of real-space potentials yield reciprocal-space structure factors. Mastering reciprocal space is essential for understanding condensed matter physics at its deepest level.

FAQ

What is the reciprocal lattice?

The reciprocal lattice is a mathematical construction where each point (hkl) corresponds to a set of crystal planes in real space. The reciprocal lattice vector g_hkl is perpendicular to the (hkl) planes and has magnitude 1/d_hkl (or 2π/d_hkl depending on convention). It transforms the problem of diffraction from geometry to simple point-matching.

What is the Ewald sphere?

The Ewald sphere is a geometric construction in reciprocal space with radius 1/λ (the wavevector magnitude). When a reciprocal lattice point lies on the sphere's surface, the Bragg condition is satisfied and diffraction occurs. Rotating the crystal rotates the reciprocal lattice, sweeping points through the sphere.

How are reciprocal vectors calculated?

In 2D, a* = 2π/(a·sin(γ)), b* = 2π/(b·sin(γ)), and γ* = 180° - γ. In 3D, a* = 2π(b×c)/V, b* = 2π(c×a)/V, c* = 2π(a×b)/V, where V is the unit cell volume. The reciprocal lattice vectors are perpendicular to pairs of real-space vectors.

Why is reciprocal space useful?

Reciprocal space simplifies diffraction analysis enormously. Instead of computing path differences for plane waves scattering off crystal planes, we simply check which reciprocal lattice points intersect the Ewald sphere. It also provides natural coordinates for describing electronic band structure, phonon dispersion, and Brillouin zones.

Sources

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