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electroweak symmetry breaking

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electroweak symmetry breaking
electroweak symmetry breaking
Cush · Public domain · source
NameElectroweak symmetry breaking
FieldParticle physics
Introduced1960s
Key figuresPeter Higgs, François Englert, Robert Brout, Gerald Guralnik, C. R. Hagen, Tom Kibble, Steven Weinberg, Abdus Salam
Major theoryStandard Model

electroweak symmetry breaking Electroweak symmetry breaking is the process in the Standard Model that differentiates the electromagnetism and weak interaction forces, giving mass to the W and Z bosons while leaving the photon massless. Developed amid work by Peter Higgs, François Englert, Robert Brout, Gerald Guralnik, C. R. Hagen, Tom Kibble, Steven Weinberg, and Abdus Salam, it ties together predictions tested at facilities such as the Large Hadron Collider, CERN, and Fermilab. The concept underpins searches and measurements by collaborations like ATLAS, CMS, ALEPH, and intersects with theoretical programs at institutions such as Institute for Advanced Study, Max Planck Society, and Perimeter Institute.

Overview and Historical Development

The historical development traces from symmetry ideas in the 1950s through electroweak unification by Sheldon Glashow and later renormalizable formulation by Gerard 't Hooft and Martinus Veltman, culminating in the 1964 independent proposals by Peter Higgs, François Englert, and Robert Brout alongside the trilogy of Guralnik, Hagen, Kibble; experiments at CERN and SLAC National Accelerator Laboratory then constrained parameters. Influential workshops and programs at Imperial College London, Princeton University, Harvard University, and University of Cambridge fostered connections between quantum field theory practitioners and experimental collaborations like LEP and Tevatron. Nobel recognitions to Peter Higgs, François Englert, and earlier prizes tied to Gerard 't Hooft reflect institutional validation from bodies such as the Royal Swedish Academy of Sciences and the Nobel Committee.

Theoretical Framework

The theoretical framework is built on gauge symmetry of the SU(2)×U(1) group realized in the Standard Model, with spontaneous symmetry breaking implemented via a scalar field in a potential akin to the Mexican hat introduced in quantum field theory texts used at MIT, Caltech, and University of Oxford. Key computations employ techniques developed by Richard Feynman, Julian Schwinger, and Sin-Itiro Tomonaga and rely on renormalization methods formalized by Gerard 't Hooft and Kenneth G. Wilson. The framework connects to perturbative expansions in calculations performed at CERN's Large Hadron Collider, lattice simulations from Brookhaven National Laboratory and RIKEN, and effective field theory approaches championed by scholars affiliated with University of Chicago and Stanford University.

Higgs Mechanism and Mass Generation

The Higgs mechanism posits a scalar field acquiring a nonzero vacuum expectation value that breaks SU(2)×U(1) symmetry and yields longitudinal polarizations for W and Z through interactions described in Lagrangians taught at Caltech and Columbia University. Mass terms for fermions arise via Yukawa couplings that link the scalar to quarks like the top quark and leptons such as the tau lepton, with coupling hierarchies explored in models from groups at CERN and Fermilab. The discovery of a 125 GeV scalar by ATLAS and CMS at Large Hadron Collider validated the mechanism in part, echoing earlier precision electroweak fits performed by collaborations at LEP and experiments led from SLAC National Accelerator Laboratory.

Experimental Evidence and Measurements

Experimental evidence includes precision tests of electroweak parameters at LEP, mass measurements at Tevatron, and the 2012 scalar discovery by ATLAS and CMS at CERN; follow-up studies involve differential cross-section analyses and coupling fits done by teams at Brookhaven National Laboratory, Fermilab, and DESY. Key observables such as the W boson mass, Z boson mass, and branching ratios for channels like diphoton and ZZ* were measured in datasets from Run 1 of the LHC, Run 2 of the LHC, and heavy-flavor experiments at KEK and Belle II. Global fits combining results from Particle Data Group compendia and analyses by collaborations at Imperial College London and University of California, Berkeley constrain potential deviations and guide searches in detector upgrades funded by agencies including the European Research Council and U.S. Department of Energy.

Beyond the Standard Model and Alternative Mechanisms

Beyond Standard Model proposals include supersymmetry envisioned by groups at University of Cambridge and Princeton University, composite Higgs scenarios developed at CERN and Johns Hopkins University, extra-dimensional models from teams at Stanford University and University of Chicago, and technicolor approaches explored at Brookhaven National Laboratory and Yale University. Experimental programs seeking signs of these alternatives run at Large Hadron Collider, future colliders proposed by panels convened under International Committee for Future Accelerators and European Strategy for Particle Physics, and neutrino facilities like Fermilab’s DUNE and Japan Proton Accelerator Research Complex. Theoretical intersections with cosmology involve groups working on inflationary scenarios at Princeton University and dark matter candidates studied by collaborations such as LUX-ZEPLIN and XENONnT.

Category:Particle physics