A phonon is a collective vibrational mode in an ideal crystalline solid.
A single phonon is pure vibrational mode. It is direct analogy to a pure vibrational mode in a musical instrument such as a string of a guitar.
It can be said that it is a sound wave, but the vibrations allowed that are pure single mode vibrations are more extensive than simple sound waves.
Phonons, in their original and normal sense, occur in perfect crystalline structures where each atom has a specific equilibrium location that is repeated regularly in space.
In a pure single phonon mode there is a periodic vibration (i.e. displacement) of each atom that is described as a sinusoidal variation in space and time. One specifies a particular phonon with a wavelength, direction and frequency, just as with a sound wave.
In real solids, there are imperfections, but they are near enough to idea that the idealized concept of a phonon is usually completely adequate.
Finally, phonons can be described as classical vibrations as is natural in classical mechanics and they can be described as quantum vibrations using quantum mechanics. The quantum description is fundamentally correct, but the classical description is very useful and convenient in many cases. Some people would say that you should not call the collective vibrations of a solid phonons unless you are describing them as a quantum phenomena but other people would say that is too picky. Usually, however, the term phonon implies that quantum nature of the vibration of a crystal.
The phonon effect refers to the interaction of electrons in a crystal lattice with lattice vibrations. This interaction can cause scattering of electrons, affecting the electrical and thermal properties of the material. Phonons play a significant role in determining the overall behavior of materials at the quantum level.
The phonon effect is the name given to pseudo particle which transmits vibrational kinetic energy through a medium. Vibrations caused by thermal energy within a crystal lattice cause phonon generation, and electron-phonon interactions are the primary cause of electrical resistance in metals. The phonon can also be viewed as a wave phenomenon when vibrations are emitted from a physical source, rather than a thermal source. If the medium for these phonon waves is air or water, it is typically referred to as sound, thereby explaining the root "phon" from the greek word for sound "phonos."
Electron-phonon interaction refers to the interaction between electrons and lattice vibrations (phonons) in a material, influencing its electronic properties. Phonon-electron interaction, on the other hand, describes the interaction between lattice vibrations and electrons, affecting the thermal and transport properties of the material. Essentially, the difference lies in the direction of the interaction, with electron-phonon focusing on the effect of lattice vibrations on electrons, and phonon-electron focusing on the effect of electrons on lattice vibrations.
Ag phonon modes refer to acoustic phonon modes where all atoms move in phase, while Bg phonon modes refer to optical phonon modes where atoms move in opposite directions. Ag modes are usually lower in energy and frequency compared to Bg modes. These modes are often used to describe the vibrational behavior of crystals in condensed matter physics.
Optical phonons are modes where the ions in the crystal lattice move in a way that involves a change in the material's polarization. These phonons interact strongly with light, leading to changes in the material's optical properties. The energy of optical phonons corresponds to the energy of photons in the optical frequency range.
the Coriolis effect
Silicon (Si) and Germanium (Ge) do not emit light because they are indirect bandgap materials. This means that when they are excited, most of the electrons and holes recombine through phonon-mediated transitions, resulting in the release of heat instead of light. In contrast, direct bandgap materials, such as gallium arsenide (GaAs), release light when electrons and holes recombine.
Electron-phonon interaction refers to the interaction between electrons and lattice vibrations (phonons) in a material, influencing its electronic properties. Phonon-electron interaction, on the other hand, describes the interaction between lattice vibrations and electrons, affecting the thermal and transport properties of the material. Essentially, the difference lies in the direction of the interaction, with electron-phonon focusing on the effect of lattice vibrations on electrons, and phonon-electron focusing on the effect of electrons on lattice vibrations.
Ag phonon modes refer to acoustic phonon modes where all atoms move in phase, while Bg phonon modes refer to optical phonon modes where atoms move in opposite directions. Ag modes are usually lower in energy and frequency compared to Bg modes. These modes are often used to describe the vibrational behavior of crystals in condensed matter physics.
The smallest unit of sound wave energy is called a phonon. Phonons are quantized units of vibrational energy in a crystal lattice or in any elastic medium which carries sound.
sound and other mechanical vibrations are quantized as bosonic particles called phonons.
Source from Wikipedia:It can be derived from "φέρειν φόνον", pherein phonon, "to bring (or cause) death".
The energy leaves as either a photon or phonon.
Lloyd W. Root has written: 'Phonon attenuation characteristics of manganous oxide (MnO)'
R. J. Nicholas has written: 'The magnetophonon effect' -- subject(s): Phonons, Electron-phonon interactions
Mark John Smith has written: 'Low temperature phonon-drag thermoelectric power calculations in GaAs/GaAlAs heterojunctions and Si MOSFETs'
Jay Charles Hicks has written: 'Electron-phonon contribution to the electronic density of states in a dilute alloy' -- subject- s -: Alloys, Analysis
Optical phonons are modes where the ions in the crystal lattice move in a way that involves a change in the material's polarization. These phonons interact strongly with light, leading to changes in the material's optical properties. The energy of optical phonons corresponds to the energy of photons in the optical frequency range.
Melanie L. Ledgerwood has written: 'Phonon dynamics and self-energy effects in highly photo-excited germanium' -- subject(s): Physics Theses 'Ultrashort period laser induced periodic surface structures' -- subject(s): Physics Theses