charm quark oor Masedonies
charm quark
en
(physics) A quark having a fractional electric charge of +2/3 and a mass about 1150 to 1350 MeV. Symbol: c
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волшебен кварк
en
type of quark
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Charm quarks are found in hadrons, which are subatomic particles made of quarks.
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They meet in the middle, and they create subatomic particles like the charm quark and the tau lepton.
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The D mesons are the lightest particle containing charm quarks.
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In collaboration with James Bjorken, Glashow was the first to predict a fourth quark, the charm quark, in 1964.
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Mesons formed by a bound state of a charm quark and a charm anti-quark are generally known as "charmonium".
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For instance a pentaquark made of two up quarks, one down quark, one charm quark, and one charm antiquark would be denoted uudcc.
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In 2017, the LHCb researchers reported yet another Xi baryon: the double charmed Ξ++ cc baryon, consisting of two heavy charm quarks and one up quark.
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With Thomas Appelquist, Politzer also played a central role in predicting the existence of "charmonium", a subatomic particle formed of a charm quark and a charm antiquark.
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Since the D mesons are the lightest mesons containing a single charm quark (or antiquark), they must change the charm (anti)quark into an (anti)quark of another type to decay.
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The subscript character, or its absence, indicates whether the third quark is a strange quark ( Λ0 ) (no subscript), a charm quark ( Λ+ c), a bottom quark ( Λ0 b), or a top quark ( Λ+ t).
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The proposal of Kobayashi and Maskawa heavily relied on the GIM mechanism put forward by Sheldon Lee Glashow, John Iliopoulos and Luciano Maiani, which predicted the existence of the then still unobserved charm quark.
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In fact, instead of suppression, enhanced production of J/ψ is expected in heavy ion experiments at LHC where the quark-combinant production mechanism should be dominant given the large abundance of charm quarks in the QGP.
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In D mesons, the charm quark preferentially changes into a strange quark via an exchange of a W particle, therefore the D meson preferentially decays into K s and π s. ^ PDG reports the resonance width (Γ).
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The prediction of the charm quark also removed a technical disaster for any quantum field theory with unequal numbers of quarks and leptons — an anomaly — where classical field theory symmetries fail to carry over into the quantum theory.
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The charmed eta meson ( η c) and bottom eta meson ( η b) are similar forms of quarkonium; they have the same spin and parity as the (light) η defined, but are made of charm quarks and bottom quarks respectively.
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These masses are on the same order of magnitude as the masses of many experimentally observed mesons and baryons, as well as to the masses of the tau lepton, charm quark, bottom quark, some hydrogen isotopes, and some helium isotopes.
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When in November 1974 teams at Brookhaven National Laboratory (BNL) and the Stanford Linear Accelerator Center (SLAC) simultaneously announced the discovery of the J/ψ meson, it was soon after identified as a bound state of the missing charm quark with its antiquark.
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In particle physics, a hyperon is any baryon containing one or more strange quarks, but no charm, bottom, or top quark.
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This is due to the requirement that the disappearance of J/ψ mesons is evaluated with respect to the baseline provided by the total production of all charm quark-containing subatomic particles, and because it is widely expected that some J/ψ are produced and/or destroyed at time of QGP hadronization.
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The quark contents of these states are almost all qqQQ, where q represents a light (up, down or strange) quark, Q represents a heavy (charm or bottom) quark, and antiquarks are denoted with an overline.
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The true analogs of positronium in the theory of strong interactions, however, are not exotic atoms but certain mesons, the quarkonium states, which are made of a heavy quark such as the charm or bottom quark and its antiquark.
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A 1970 idea of Sheldon Glashow, John Iliopoulos, and Luciano Maiani, known as the GIM mechanism, showed that the flavor-changing decays would be strongly suppressed if there were a fourth quark, charm, that paired with the strange quark.
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There are six quarks (up, down, strange, charm, bottom and top quarks), and six leptons (electron, electron neutrino, muon, muon neutrino, tau particle and tau neutrino), along with the corresponding antiparticle of each of these.
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The much larger mass differences between the charm and bottom quarks and the lighter quarks results in states that are well defined in terms of a quark–antiquark pair of a given flavor.
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Xi baryons, in particular, contain one up or down quark plus two more massive quarks: either strange, charm or bottom.
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30 sinne gevind in 7 ms. Hulle kom uit baie bronne en word nie nagegaan nie.