background radiation tâbeš-e paszaminé, ~ zaminé Fr.: rayonnement du fond The isotropic residual microwave radiation in space left from the primordial → Big Bang. Same as → cosmic microwave background (CMB) radiation. → background; → radiation. |
blackbody radiation tâbeš-e siyah-jesm (#) Fr.: rayonnement de corps noir The radiation emitted by a blackbody at a given → temperature. The → distribution of radiation with → wavelength is given by → Planck's blackbody formula or → Planck's radiation law. |
Cherenkov radiation tâbeš-e Čerenkov (#) rayonnement de Čerenkov Visible radiation emitted when → charged particles pass through a transparent medium faster than the speed of light in that medium. Named after Pavel A. Čerenkov (1904-1990), Russian physicist, who discovered the phenomenon. He shared the Nobel prize 1958 in physics with Ilya Frank and Igor Tamm, who in 1937 gave the theoretical explanation for this radiation. |
corpuscular radiation tâbeš-e karpuli Fr.: rayonnement corpusculaire A stream of atomic or subatomic particles. |
cosmic background radiation tâbeš-e paszaminé-ye keyhâni Fr.: rayonnement du fond cosmique → cosmic microwave background radiation (CMBR). → cosmic; → background; → radiation. |
cosmic microwave background radiation (CMBR) tâbeš-e rizmowj-e paszaminé-ye keyhâni Fr.: rayonnement du fond cosmique microonde The diffuse → electromagnetic radiation in the → microwave band, coming from all directions in the sky, which consists of relic photons left over from the very hot, early phase of the → Big Bang. More specifically, the CMBR belong to the → recombination era, when the → Universe was about 380,000 years old and had a temperature of about 3,000 K, or a → redshift of about 1,100. The photons that last scattered at this epoch have now cooled down to a temperature of 2.73 K. They have a pure → blackbody spectrum as they were at → thermal equilibrium before → decoupling. The CMB was discovered serendipitously in 1965 by Penzias and Wilson (ApJ L 142, 419) and was immediately interpreted as a relic radiation of the Big Bang by Dicke et al. (1965, ApJL 142, 383). Such a radiation had been predicted before by Gamow (1948, Nature 162, 680) and by Alpher and Herman (1948, Nature 162, 774). This discovery was a major argument in favor of the Big Bang theory. In 1992, the satellite → Cosmic Background Explorer (COBE) discovered the first anisotropies in the temperature of the CMB with an amplitude of about 30 µK. See also: → cosmic microwave background anisotropy, → dipole anisotropy, → CMB lensing, → CMB angular power spectrum, → acoustic peak, → baryon acoustic oscillation, → WMAP. → cosmic; → microwave; → background; → radiation. |
dipole radiation tâbeš-e doqotbé Fr.: rayonnement dipolaire The electromagnetic radiation produced by an oscillating → electric dipole or → magnetic dipole. |
electromagnetic radiation tâbeš-e barqâmeqnâti Fr.: rayonnement électromagnétique Radiation propagating in the form of an advancing wave in electric and magnetic fields. It includes radio waves, infrared, visible light, ultraviolet, X-rays, and gamma rays. → electromagnetic; → radiation. |
gravitational radiation tâbeš-e gerâneši (#) Fr.: rayonnement gravitationnel The → energy transported by → gravitational waves. Gravitational radiation is to → gravity what light is to → electromagnetism. → gravitational; → radiation. |
Hawking radiation tâbeš-e Hawking (#) Fr.: rayonnement de Hawking The radiation produced by a → black hole when → quantum mechanical effects are taken into account. According to quantum physics, large fluctuations in the → vacuum energy occurs for brief moments of time. Thereby virtual particle-antiparticle pairs are created from vacuum and annihilated. If → pair production happens just outside the → event horizon of a black hole, as soon as these particles are formed they would both experience drastically different → gravitational attractions due to the sharp gradient of force close to the black hole. One particle will accelerate toward the black hole and its partner will escape into space. The black hole used some of its → gravitational energy to produce these two particles, so it loses some of its mass if a particle escapes. This gradual loss of mass over time means the black hole eventually evaporates out of existence. See also → Bekenstein formula, → Hawking temperature. Named after the British physicist Stephen Hawking (1942-2018), who provided the theoretical argument for the existence of the radiation in 1974; → radiation. |
infrared radiation tâbeš-e forusorx (#) Fr.: rayonnement infrarouge That part of the → electromagnetic radiation lying beyond the red, between the radio and the visible regions of the → electromagnetic spectrum. The wavelengths range from about 0.8 → microns (μm) to about 1000 μm. See also: → near-infrared; → mid-infrared; → far-infrared; → submillimeter radiation. |
intensity of radiation datanuyi-e tâbeš Fr.: intensité de rayonnement The rate of emitted energy from unit surface area through unit solid angle. The radiation from a surface has different intensities in different directions. |
interstellar radiation field meydân-e tâbeš andaraxtari Fr.: champ de rayonnement interstellaire A global ionizing radiation in the → interstellar medium provided by various sources all together. → interstellar; → radiation; → field. |
ionizing radiation tâbeš-e yonandé (#) Fr.: rayonnement ionisant A photon that has enough energy to remove an electron from an atom or molecule, thus producing an ion and free electrons. |
irradiation 1) tâbešdehi, tâbešgiri; 2) nurgostard Fr.: irradiation 1) Exposure to any kind of radiation or atomic particles. Irradiation, from ir- variant of → in- (by assimilation) before r + → radiation. 1) Tâbešdehi, tâbešgiri;, from tâbeš→ radiation + giri verbal noun of gereftan
"to take, seize" (Mid.Pers. griftan, Av./O.Pers. grab-
"to take, seize," cf.
Skt. grah-, grabh- "to seize, take," graha
"seizing, holding, perceiving," M.L.G. grabben "to grab,"
from P.Gmc. *grab, E. grab "to take or grasp suddenly;"
PIE base *ghrebh- "to seize"); dahi verbal noun of dâdan
"to give," Mid.Pers. dâdan "to give" (O.Pers./Av. dā-
"to give, grant, yield,"
dadāiti "he gives;" Skt. dadáti "he gives;"
Gk. tithenai "to place, put, set," didomi "I give;"
L. dare "to give, offer," facere "to do, to make;"
Rus. delat' "to do;" O.H.G. tuon, Ger. tun,
O.E. don "to do;" PIE base *dhe- "to put, to do"). |
magnetic-dipole radiation tâbeš-e doqotbe-ye meqnâtisi (#) Fr.: rayonnement du dipôle magnétique Radiation emitted by a rotating magnet. |
microwave background radiation tâbeš-e paszamine-ye rizmowj Fr.: rayonnement micro-onde du fond cosmique Thermal radiation with a temperature of 2.73 K that is apparently uniformly distributed in the Universe. It is believed to be a redshifted remnant of the hot radiation that was in thermal equilibrium with matter during the first hundred thousand years after the Big Bang. Same as → cosmic microwave background (CMB) radiation. → microwave; → background; → radiation. |
microwave radiation tâbeš-e rizmowj (#) Fr.: rayonnement micro-onde Electromagnetic radiation carried by → microwaves. |
non-coherent radiation tâbeš-e nâhamdus (#) Fr.: rayonnement incohrént Radiation having waves that are out of phase in space and/or time; radiation which is not → coherent. |
non-thermal radiation tâbeš-e nâgarmâyi (#) Fr.: rayonnement non thermique The electromagnetic radiation whose characteristics do not depend on the temperature of the emitting source. In contrast to → thermal radiation, it has a different spectrum from that of → blackbody radiation. The three common types of non-thermal radiation in astronomy are: → synchrotron radiation, → bremsstrahlung radiation, and → maser → stimulated emission. → non-thermal; → radiation. |