
A lattice structure that prevents light from scattering and forces it to circulate, enabling light confinement.A photonic crystal is an optical material with a periodic variation in its refractive index, arranged on a scale comparable to the wavelength of light. This structure creates a 'photonic band gap' — a range of frequencies for which light cannot propagate through the material, much like the electronic band gap in semiconductors prevents electrons from moving at certain energies. As a result, light is forced to take specific paths, can be confined in tiny volumes, or can be manipulated to flow around sharp corners without scattering.
The concept was independently proposed by Eli Yablonovitch and Sajeev John in 1987, drawing on the analogy between electron waves in periodic potentials and light waves in periodic dielectrics.
The periodic arrangement acts as a Bragg mirror in all directions: at each interface, light reflections interfere destructively for certain wavelengths, canceling the forward wave. For frequencies inside the band gap, no propagating modes exist, so light is either reflected or, if a defect is introduced (like a missing rod or a line of altered holes), it becomes trapped in that defect and can only travel along it. This allows waveguides with bends that would normally leak light, or microcavities that confine light to volumes smaller than the wavelength.
Photonic crystals are used in optical fibers with a hollow core (photonic-crystal fibers), in compact laser cavities, and in integrated photonic circuits for routing light on chips.
The first photonic crystal operating at microwave frequencies was nicknamed 'Yablonovite' after its inventor, and it was made by drilling a triangular array of holes into a dielectric slab.







