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Phononic Band Gap

Dispersion relation for a 1D diatomic lattice

Parameters

Science

A 1D diatomic chain has alternating masses M₁ and M₂ coupled by spring constant k. The dispersion relation has two branches:

ω±² = k(1/M₁+1/M₂) ± k√[(1/M₁+1/M₂)²−4sin²(qa/2)/(M₁M₂)]

The band gap opens at the Brillouin zone boundary q=π/a:

Δω = ω₊(π/a) − ω₋(π/a) = √(2k/M₁) − √(2k/M₂)

In the acoustic branch, M₁ and M₂ move in phase. In the optical branch, they move out of phase — this couples to light in ionic crystals.