Down quark: Difference between revisions

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|discovered = [[SLAC]] (1968)
|symbol = {{SubatomicParticle|Down quark}}
|mass = 34.5–1-{{val|65.08|ul=MeVGeV/c2}}<ref name="PDG2009PDG2010">
{{cite web
|author=CK. AmslerNakamura ''et al.'' ([[Particle Data Group]])
|url=http://pdglivepdg.lbl.gov/Rsummary2010/tables/rpp2010-sum-quarks.brl?nodein=Q001pdf
|title=PDGLive Particle Summary 'Quarks (u, d, s, c, b, t, b', t', Free)'
|publisher=[[Particle Data Group]]
|year=20092010
|accessdate=20092010-0708-2311
}}</ref>
 
|decay_time =
|decay_particle = [[Up quark]]
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}}
 
The '''down quark''' or '''d quark''' (from its symbol, ''d'') is the second-lightest of all [[quark]]s, a type of [[elementary particle]], and a major constituent of [[matter]]. It, along with the [[up quark]], forms the [[neutron]]s (one up quark, two down quarks) and [[proton]]s (two up quarks, one down quark) of [[atomic nucleus|atomic nuclei]]. It is part of the [[generation (physics)|first generation]] of matter, has an [[electric charge]] of −{{frac|1|3}}&nbsp;[[elementary charge|e]] and a [[Quark#Mass|bare mass]] of 34.5–1–{{val|65.08|ul=MeV/c2}}.<ref name="PDG2010"/> Like all [[quark]]s, the down quark is an [[elementary particle|elementary]] [[fermion]] with [[spin (physics)|spin]]-[[spin-1/2|{{frac|1|2}}]], and experiences all four [[fundamental interaction]]s: [[gravitation]], [[electromagnetism]], [[weak interaction]]s, and [[strong interaction]]s. The [[antiparticle]] of the down quark is the '''down antiquark''' (sometimes called ''antidown quark'' or simply ''antidown''), which differs from it only in that some of its properties have [[additive inverse|equal magnitude but opposite sign]].
 
Its existence (and that of the [[up quark|up]] and [[strange quark]]s) was postulated in 1964 by [[Murray Gell-Mann]] and [[George Zweig]] to explain the ''[[Eightfold Way (physics)|Eightfold Way]]'' classification scheme of [[hadron]]s. The down quark was first observed by experiments at the [[Stanford Linear Accelerator Center]] in 1968.
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==Mass==
 
Despite being extremely common, the 'bare' [[Quark#Mass|bare mass]] of the down quark is not well determined, but probably lies between 34.51 and {{val|6.5.8|ul=MeV/c2}}.<ref name="PDG2009PDG2010"/> When found in [[mesons]] (particles made of one quark and one [[antiparticle|antiquark]]) or [[baryon]]s (particles made of three quarks), the 'effective mass' (or 'dressed' mass) of quarks [[Quark#Mass|becomes greater]] because of the [[Quantum chromodynamics binding energy|binding energy]] caused by the [[gluon|gluon field]] between each quarks (see [[mass–energy equivalence]]). For example, the effective mass of down quarks in a proton is around {{val|330|u=MeV/c2}}. Because the bare mass of down quarks is so light, it cannot be straightforwardly calculated because relativistic effects have to be taken into account.
 
== See also ==