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top quark

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Parent: Higgs boson Hop 3
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1. Extracted63
2. After dedup14 (None)
3. After NER7 (None)
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top quark
top quark
Raeky · Public domain · source
NameTop quark
GenerationThird
Charge+2/3 e
Mass172.76 GeV/c^2 (approx.)
Spin1/2
ColorTriplet
Discovered1995
Discovered atFermilab
DiscoverersCDF and DØ collaborations

top quark The top quark is the third-generation up-type elementary fermion in the Standard Model, notable for its exceptionally large mass and rapid weak decay. It plays a central role in precision tests performed at facilities such as Fermilab, CERN, and drives sensitivity to physics probed by experiments like ATLAS and CMS. The particle's properties influence theoretical constructs involving the Higgs boson, electroweak symmetry breaking, and potential extensions including supersymmetry, composite Higgs models, and extra dimensions.

Introduction

The top quark occupies the up-type position in the third generation alongside the bottom quark and is a member of the quark model framework used by formulations from Murray Gell-Mann and George Zweig. Predicted by patterns in the Cabibbo–Kobayashi–Maskawa matrix and the requirement of anomaly cancellation in the Glashow–Iliopoulos–Maiani mechanism, its discovery completed the third family predicted in the context of the Electroweak theory developed by Sheldon Glashow, Abdus Salam, and Steven Weinberg. Experimental confirmation was achieved by the Collider Detector at Fermilab (CDF) and collaborations at the Tevatron accelerator under directorates associated with Fermilab leadership and supported by agencies such as the U.S. DOE and the National Science Foundation.

Properties

The top quark has spin 1/2 and carries a color charge under Quantum chromodynamics as a color triplet, coupling to gluons described by Quantum chromodynamics (QCD). Its electric charge is +2/3 e, the same as the up quark and charm quark, and its mass, measured in analyses by ATLAS, CMS, and Tevatron experiments, is approximately 173 GeV/c^2, comparable to a gold nucleus mass scale and far heavier than the bottom quark or tau lepton. The Yukawa coupling between the top quark and the Higgs boson is near unity, influencing radiative corrections in precision fits carried out by collaborations working with the Large Hadron Collider and laboratories like CERN and DESY. The top quark's short lifetime, shorter than hadronization timescales predicted by QCD confinement arguments, prevents formation of top-flavored hadrons in typical conditions explored at colliders overseen by institutions such as Brookhaven National Laboratory and the SLAC National Accelerator Laboratory.

Production and Decay

Top quarks are predominantly produced in pairs via strong interactions at hadron colliders through partonic processes computed using perturbative Quantum chromodynamics with parton distribution functions from groups like CTEQ, NNPDF, and MMHT. Single top production proceeds through electroweak channels mediated by the W boson via t-channel, s-channel, and associated tW production modes studied by the CDF, , ATLAS, and CMS collaborations. The dominant decay mode is t → Wb, coupling governed by elements of the CKM matrix particularly |V_tb|, with subsequent W decays producing lepton+jets, dilepton, and all-hadronic final states analyzed in searches by teams at Tevatron and Large Hadron Collider experiments. Higher-order corrections, including next-to-leading-order and next-to-next-to-leading-order computations, are provided by theory groups associated with Les Houches workshops and software such as MadGraph, POWHEG, and MCFM.

Experimental Detection and Measurement

Precision measurements of the top quark mass, cross sections, spin correlations, and couplings have been performed by experimental collaborations like CDF, , ATLAS, and CMS using detectors located at facilities including Tevatron and the Large Hadron Collider. Techniques include kinematic reconstruction, matrix-element methods, and template fits developed in analyses guided by statistical frameworks championed by groups at CERN and the Particle Data Group; systematic uncertainties are controlled through calibration with samples from Z boson and W boson processes and constrained by parton shower models from PYTHIA and HERWIG. Measurements of single top production established |V_tb| constraints and enabled tests of anomalous couplings searched for by collaborations collaborating with funding agencies like the European Research Council and national laboratories such as Fermilab.

Role in the Standard Model and Beyond

The top quark contributes significantly to loop corrections in electroweak precision observables measured at experiments including LEP and SLD, affecting fits that constrain the Higgs boson mass prior to its discovery and informing global analyses by the Particle Data Group. Its large Yukawa coupling makes it central to theories addressing naturalness problems posed by radiative corrections to the Higgs mass, motivating proposals such as supersymmetry, composite Higgs models, Little Higgs models, and scenarios with extra dimensions investigated by theorists affiliated with institutions like Institute for Advanced Study and Princeton University. Searches for flavor-changing neutral currents involving the top quark, and for rare decays predicted in models by groups at CERN and KEK, provide sensitive probes of physics beyond the Standard Model pursued by collaborations across global accelerator programs.

Historical Discovery and Research Developments

The search for the top quark followed the discovery of the bottom quark and the formulation of the three-generation quark picture by figures including Kobayashi and Maskawa; experimental hints were pursued in fixed-target and collider programs at CERN SPS, DESY, and SLAC. The definitive observation in 1995 by the CDF and collaborations at Fermilab culminated decades of theoretical and experimental effort led by institutions such as Brookhaven National Laboratory and universities worldwide. Subsequent research at the Tevatron refined mass and cross-section measurements, while the Large Hadron Collider era, with experiments ATLAS and CMS, expanded precision studies, electroweak tests, and searches for new phenomena connected to the top quark, with ongoing work coordinated through collaborations and workshops held at CERN and international conferences like ICHEP and Moriond.

Category:Elementary particles