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top quark
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(physics) A quark having a fractional electric charge of +2/3 and a mass about 178,000 MeV. Symbol: t
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The top quark Yukawa coupling lies very near the infrared fixed point of the Standard Model.
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The top quark is too heavy to form a similar meson, due to its very fast decay.
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A distinctly different process is the production of single top quarks via weak interaction.
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Because top quarks are very massive, large amounts of energy are needed to create one.
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The top quark interacts primarily by the strong interaction, but can only decay through the weak force.
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The Higgs boson has a Yukawa coupling to the left- and right-handed top quarks.
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(Top quarks are so heavy that they decay through the weak force before they can form bound states.)
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Early searches for the top quark at SLAC and DESY (in Hamburg) came up empty-handed.
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This is used to make measurements of the mass of particles like the Z boson or the top quark.
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The top quark was sometimes called truth quark in the past, but over time top quark became the predominant use.
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In particle physics, a stop squark, symbol t͂ , is the superpartner of the top quark as predicted by supersymmetry (SUSY).
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In the Standard Model, the top quark is predicted to have a spin quantum number of 1⁄2 and electric charge +2⁄3.
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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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In the Standard Model, all of the quark and lepton Yukawa couplings are small compared to the top quark Yukawa coupling.
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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 value of the fixed point is fairly precisely determined in the Standard Model, leading to a top quark mass of 230 GeV.
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The combination of a bottom antiquark and a top quark is not thought to be possible because of the top quark's short lifetime.
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The top quark, also known as the t quark (symbol: t) or truth quark, is the most massive of all observed elementary particles.
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The W bosons from top quark decays carry polarization from the parent particle, hence pose themselves as a unique probe to top polarization.
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The Tevatron was (until the start of LHC operation at CERN in 2009) the only hadron collider powerful enough to produce top quarks.
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Because of its enormous mass, the top quark is extremely short-lived with a predicted lifetime of only 6975500000000000000♠5×10−25 s.
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A first measurement of the top quark charge has been published, resulting in approximately 90% confidence limit that the top quark charge is indeed +2⁄3.
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Since then, confirmation of the top quark (1995), the tau neutrino (2000), and the Higgs boson (2012) have added further credence to the Standard Model.
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The W and Z bosons decay to fermion–antifermion pairs but neither the W nor the Z bosons can decay into the higher-mass top quark.
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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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