bottom quark oor Masedonies
bottom quark
en
(physics) A quark having a fractional electric charge of -1/3 and a mass about 4,100 to 4,400 MeV. Symbol: b
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длабински кварк
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type of quark
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Among his achievements are the discovery of the muon neutrino in 1962 and the bottom quark in 1977.
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The uncertainty in this prediction arises because the bottom quark Yukawa coupling can be amplified in the MSSM.
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The bottom quark was first described theoretically in 1973 by physicists Makoto Kobayashi and Toshihide Maskawa to explain CP violation.
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A single top quark can also be produced in association with a W boson, requiring an initial state bottom quark ("tW-channel").
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The combination of a bottom antiquark and a bottom quark is not a B meson, but rather bottomonium which is something else entirely.
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However a Ξ0 b contains one up, one strange, and one bottom quark, while a Ξ0 bb contains one up and two bottom quarks.
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It decays to a W boson and either a bottom quark (most frequently), a strange quark, or, on the rarest of occasions, a down quark.
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It was the first known particle made of quarks from all three quark generations – namely, a down quark, a strange quark, and a bottom quark.
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However, the speed of the charm and the bottom quarks in their respective quarkonia is sufficiently smaller, so that relativistic effects affect these states much less.
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The bottom quark is also notable because it is a product in almost all top quark decays, and is a frequent decay product of the Higgs boson.
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Kobayashi and Maskawa won the 2008 Nobel Prize in Physics for the prediction of the top and bottom quark, which together form the third generation of quarks.
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The Yukawa couplings of the up, down, charm, strange and bottom quarks, are hypothesized to have small values at the extremely high energy scale of grand unification, 1015 GeV.
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Kobayashi and Maskawa's theory required that there were at least three generations of quarks, a prediction that was confirmed experimentally four years later by the discovery of the bottom quark.
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Maskawa and Kobayashi's theory required that there be at least three generations of quarks, a prediction that was confirmed experimentally four years later by the discovery of the bottom quark.
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The Υ(1S) state was discovered by the E288 experiment team, headed by Leon Lederman, at Fermilab in 1977, and was the first particle containing a bottom quark to be discovered.
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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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CDF physicists have previously measured the rate of the matter-antimatter transitions for the B_s meson, which consists of the heavy bottom quark bound by the strong nuclear interaction to a strange antiquark.
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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 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 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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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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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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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 can happen in several ways (called channels): either an intermediate W-boson decays into a top and antibottom quark ("s-channel") or a bottom quark (probably created in a pair through the decay of a gluon) transforms to a top quark by exchanging a W-boson with an up or down quark ("t-channel").
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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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31 sinne gevind in 7 ms. Hulle kom uit baie bronne en word nie nagegaan nie.