fônons

Fônons, or phonons in English, are quantized collective excitations of the vibrational modes of atoms in a crystalline solid. They arise when the normal modes of lattice vibrations are treated within quantum mechanics, so the vibration energy is carried by discrete quasiparticles called phonons. Each phonon is characterized by a wavevector and a frequency, and the energy is proportional to h-bar times the angular frequency.

In a crystal with N atoms in its primitive cell, there are 3N phonon branches corresponding to the different vibrational modes. These branches split into acoustic and optical types. Acoustic phonons involve in-phase motions of atoms and dominate long-wavelength vibrations, while optical phonons involve out-of-phase motions of atoms within the basis and can have finite energy even at zero wavevector. The relation between frequency and wavevector, or dispersion relation, determines how phonons transport energy and interact with other excitations. At long wavelengths, acoustic phonons often follow omega proportional to k, reflecting sound-wave behavior; optical phonons typically have nonzero frequencies at k = 0.

Phonons play a central role in many material properties. They govern heat capacity and thermal conductivity; at low temperatures, the Debye model describes their contribution to heat capacity. Phonon scattering processes—phonon-phonon, phonon-electron, and scattering by impurities or defects—shape thermal transport and electronic behavior in solids. Phonons also couple to electrons, an interaction essential to conventional superconductivity and to various electronic, optical, and thermoelectric phenomena. Experimental methods such as inelastic neutron scattering, Raman spectroscopy, and infrared spectroscopy probe phonon spectra and dynamics.

Note: fônons is the Welsh term often used for phonons, with the same physical meaning.