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Hubble-Lemaitre tension taneš-e pâyâ-ye Hubble-Lemaître Fr.: Tension sur la constante de Hubble-Lemaître The discrepancy between the value of the → Hubble-Lemaitre constant inferred from a ΛCDM fit (→ Lambda cold dark matter model) to the → cosmic microwave background (CMB) and local measurements. The Universe appears to be expanding much faster now than predicted even with our latest understanding of its initial conditions and contents. Based on the → Hubble Space Telescope observations, the Hubble-Lemaitre constant is very recently estimated to be 74.03 km s-1 Mpc-1. This value indicates that the Universe is expanding at a rate about 9% faster than that implied by the → Planck satellite's observations of the → early Universe, which give a value for the Hubble constant of 67.4 km s-1 Mpc-1. For discussion, see D'Arcy Kenworthy et al. (2019, ApJ 875, 145). |
Humboldt current jarayân-e Humboldt (#) Fr.: courant de Humboldt A cold ocean current that flows northward along the western side of South America, offshore Chile and Peru. Dominate weather in this area includes coastal fog and low clouds. The presence or lack of this current is a vital part of the weather pattern known as El Niño. Named after the German naturalist and explorer Alexander von Humboldt (1769-1859). → current. |
Humphreys series seri-ye Humphreys Fr.: série de Humphreys A series of → spectral lines in the → infrared spectrum of → neutral hydrogen emitted by electrons in → excited states transitioning to the level described by the → principal quantum number n = 6. It begins at 12368 nm (Hu α 12.37 microns) and has been traced to 3281.4 nm (3.28 microns). Named after Curtis J. Humphreys (1898-1986), American physicist; → series. |
Humphreys-Davidson limit hadd-e Humphreys-Davidson Fr.: limite de Humphreys-Davidson An empirical upper → luminosity boundary in the → H-R diagram. It consists of two sections, a sloping part and a horizontal part. The sloping part, which decreases with decreasing → effective temperature, corresponds roughly to the → Eddington limit. The horizontal part is the temperature-independent upper luminosity limit for late-type → hypergiants. It is thought that → massive stars above the Humphreys-Davidson limit encounter an → instability, possibly due to the opacity-modified Eddington limit, and experience high → mass loss episodes which prevent their evolution to cooler temperatures. → Luminous Blue Variable stars are examples of this high mass loss phase. Named after Roberta M. Humphreys and Kris Davidson, who first dealt with this limit (1979, ApJ 232, 409); → limit. |
hundred sad (#) Fr.: cent The smallest three digit number in the decimal system and the smallest square of a two-digit number (10). Hundred, from O.E. hundred "a counting of 100," from P.Gmc. *hunda- "hundred," as below, + *rath "reckoning, number." Sad "hundred," from Mid.Pers. sad, sat, Av. sata- "hundred," satô.raocana- "with a hundred windows," satô.təmô.sata- "hundreds of hundred;" cf. Skt. śatá- "hundred;" Gk. hekaton; L. centum; Lith. simtas; P.Gmc. *hunda- "hundred" (Goth. hund; O.H.G. hunt); PIE *kmtom "hundred." |
Huygens Region nâhiye-ye Huygens Fr.: région de Huygens The inner bright part of the → Orion Nebula, from which most of the radiation is emitted. It is about 5' across corresponding to 0.7 pc (for a distance of 440 pc). See O'Dell (2001, ARAA 39, 99). Named after the Dutch astronomer Christiaan → Huygens (1629-1695), who sketched the appearance of the Orion Nebula. His drawing, the first such known sketch, was published in Systema Saturnium in 1659. First named such by O. Gingerich (1982, Ann. NY Acad. Sci. 395, 308); → region. |
Huygens-Fresnel principle parvaz-e Huygens-Fresnel Fr.: principe Huygens-Fresnel A development of → Huygens' principle stating that every point on a → wavefront acts, at a given instant, as a source of outgoing secondary spherical waves. The secondary wavelets mutually interfere and the resulting net light amplitude at any position in the outgoing wavefront is the vector sum of the amplitudes of all the individual wavelets. Using this principle, Fresnel calculated with a high accuracy the distribution of light in → diffraction patterns. The Huygens-Fresnel principle was put on a firm theoretical basis by Kirchhoff and expressed as an integral derived from the → wave equation. → Huygens; → Fresnel diffraction; → principle. |
hydrosphere âbsepehr (#) Fr.: hydrosphère A term denoting the water portion of the Earth's surface. |
hydrostatic pressure fešâr-e hidrotavânik Fr.: pression hydrodynamique The term ρgz in the → Bernoulli equation. It is not pressure in a real sense, because its value depends on the reference level selected. → hydrostatic; → pressure. |
hyperfine structure sâxtâr-e abar-nâzok (#) Fr.: structure hyperfine In spectroscopy, the → splitting of a spectral line into a number of very thin components. It results from a small perturbation in the energy levels of atoms or molecules due to the magnetic dipole-dipole interaction arising from the interaction of the nuclear → magnetic moment with the → spin of the electron. It can be observed only at high spectral dispersion. → fine structure. |
hysteresis pasmând (#) Fr.: hystérésis The phenomenon exhibited by a body (especially a ferromagnetic or
imperfectly elastic material) in reacting to changes in the
forces, especially magnetic forces, affecting it. Hysteresis, from Gk. hysteresis "being behind or late," from hystere-, stem of hysterein "to come late, lag behind" + -sis a suffix forming abstract nouns of action. Pasmând "lagging behind," from pas "behind" (Mid.Pers. pas "behind, before, after;" O.Pers. pasā "after;" Av. pasca "behind (of space); then, afterward (of time);" cf. Skt. pazca "behind, after, later," L. post "behind, in the rear; after, afterward;" O.C.S. po "behind, after;" Lith. pas "at, by;" PIE *pos-, *posko-) + mând stem of mândan "to remain; to be fatigued," mân "house, family" (Mid.pers. mândan "to remain, stay;" O.Pers. mān- "to remain, dwell;" Av. man- "to remain, dwell; to wait;" cf. Gk. menein "to remain;" L. manere "to stay, remain, abide," mansio "a staying, a remaining, night quarters, station" (Fr. maison, ménage; E. manor, mansion, permanent); PIE *men- "to remain, wait for." |
hysteresis loop gerdâl-e pasmând Fr.: cycle d'hystérésis A closed curve showing the change in magnetic induction of a ferromagnetic body to which an external field is applied as the intensity of this field is varied from +Hs to -Hs and back again, where Hs is the magnetic field intensity corresponding to saturation. → hysteresis; → loop. |
hysteresis loss dastraft-e pasmândi Fr.: perte par hystérésis Dissipation of energy which occurs, due to magnetic hysteresis, when the magnetic material is subject to changes of magnetization. → hysteresis; → loss. |
ice accretion farbâl-e yax Fr.: accrétion de glace Meteo.: The process by which a layer of ice builds up on solid objects that are exposed to freezing precipitation or to supercooled fog or cloud droplets. |
ignition temperature damâ-ye girâneš Fr.: température d'inflammation The minimum temperature to which a fuel must be heated in order to initiate self sustained combustion independent of another heat source. → ignition; → temperature. |
ignore nâdidé engâštan (#) Fr.: ignorer, négliger To set aside, e.g. → ignorable coordinate. From Fr. ignorer, from L. ignorare "not to know, disregard," from ignarus "not knowing, unaware," from in- "not," → un-, + gnarus "aware, acquainted with," related to gnoscere "to → know". Nâdidé engâštan literally "supposed not seen," from nâdidé "not seen" (from nâ- "not," → un- + didé "seen," p.p. of didan "to see," → sight) + engâštan "to suppose" (→ hypothesis). |
image resolution vâgošud-e vine, ~ tasvir Fr.: résolution d'image The separation between two detached but adjacent points in an image. → image; → resolution. |
image restoration bâzsâzi-ye vine, ~ tasvir (#) Fr.: restauration d'image The process by virtue of which the original image can be created by removing the blurring and the noise that occur during image formation. → image; → restoration. |
Imaging Atmospheric Cherenkov Technique (IACT) tašnik-e vinagari-ye Čerenkov-e javvi Fr.: téchnique d'imagerie Čerenkov atmosphérique The method used to detect very brief flashes of → Cherenkov radiation generated by the → cascade shower of → relativistic charged particles produced when a very high-energy → gamma ray (in the range 50 GeV to 50 TeV) strikes the atmosphere at a typical altitude of 10 km. Owing to this technique, it possible to discriminate cosmic gamma rays from the cosmic ray background and to determine their energy and source direction. More specifically, the incoming gamma-ray photon undergoes → pair production in the vicinity of the nucleus of an atmospheric molecule. The electron-positron pairs produced are of extremely high energy and immediately radiate in a → bremsstrahlung process. This radiation is itself extremely energetic, with many of the photons undergoing further pair production. A cascade of charged particles ensues which, due to its extreme energy, produces a flash of Cherenkov radiation lasting between 5 and 20 nano-seconds. The total area on the ground illuminated by this flash corresponds to many hundreds of square meters, which is why the effective area of IACT telescopes should be large. → imaging; → atmospheric; → Cherenkov; → technique. |
imperare (L.) parmâtidan Fr.: inperare (L.) Latin verb meaning "to command, rule, reign." L. imperare "to command, give orders, exercise authority," from → in- "into, in" + parare "to make ready, supply, order," related to parire "produce, give birth to," from PIE root *pere- "to produce, procure;" cf. Skt. prthukah "child, calf, young of an animal;" Gk. poris "calf, bull;" Czech spratek "brat, premature calf;" Lith. periu, pereti "to brood;" O.H.G. farro, Ger. Farre, Du. varre "bull," O.E. fearr "bull;" see below for possible Iranian cognates. Parmâtidan, from BMP plm'(d)y "to command, order," Sogd. framat- "to command," variants of farmudan, farmâyidan "to command, to order," ultimately from prefixed Proto-Ir. *fra-maH-, from *maH- "to measure," → experiment. |
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