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canonical quantum electrodynamics in covariant gauges
canonical quantum electrodynamics in covariant gauges

... we can mention the Coulomb gauge 2 , the axial gauge 3 , and the Valati n gauge 4 . In the case of the covariant gauges the above mentioned difficulty i s usually overcome by adding a term (a ...
Microscopic Realization of 2-Dimensional Bosonic Topological
Microscopic Realization of 2-Dimensional Bosonic Topological

... The sign change of b02 under time reversal can be compensated by a gauge transformation b02 → −b02 . When averaging all the gauge fluctuations, the vortex condensate has a zero expectation value hb02 i = 0 [44]. In this way, we conclude that time reversal symmetry in not broken in the ground state e ...
Discrete Symmetries
Discrete Symmetries

Higgs Colliquium, U of South Carolina - Physics
Higgs Colliquium, U of South Carolina - Physics

A G2-QCD neutron star
A G2-QCD neutron star

... fermionic baryons, especially neutrons, and have rather similar features as QCD itself. A theory with these feature is G2 -QCD, i. e. QCD where the gauge group SU(3) is replaced by the exceptional Lie group G2 [14, 15], see [16] for a review of the properties of this theory. A rough outline of the f ...
Desperately Seeking SUSY h (University of Cambridge) Please ask questions while I’m talking
Desperately Seeking SUSY h (University of Cambridge) Please ask questions while I’m talking

Issues in verification of ALPGEN heavy flavor production
Issues in verification of ALPGEN heavy flavor production

Effective Field Theory, Past and Future
Effective Field Theory, Past and Future

Monday, Nov. 27, 2006 - UTA High Energy Physics page.
Monday, Nov. 27, 2006 - UTA High Energy Physics page.

phys3313-fall12-112812
phys3313-fall12-112812

... Elementary Particle Interactions • How do these particles interact?? – All particles, including photons and neutrinos, participate in ...
Seiberg-Witten Theory and Calogero
Seiberg-Witten Theory and Calogero

Thermodynamics of the high temperature Quark-Gluon - IPhT
Thermodynamics of the high temperature Quark-Gluon - IPhT

... of a weak coupling calculation in thermal field theories is not only the strength of the coupling, but also the magnitude of the thermal fluctuations. These vary according to the relevant momentum scales, so that the accuracy of the weak coupling expansion depends on which momentum scale contribute ...
Effective Field Theories, Reductionism and Scientific Explanation
Effective Field Theories, Reductionism and Scientific Explanation

... considered to be an effective field theory (EFT). Particle physicists, for example, even take a supposed-to-be fundamental theory such as the celebrated Standard Model of the electromagnetic, weak, and strong interactions to be an EFT (Meissner, 1992). Nuclear physicists systematically derive low-ener ...
Atomic matter of nonzero-momentum Bose-Einstein condensation and orbital current order
Atomic matter of nonzero-momentum Bose-Einstein condensation and orbital current order

... frequency on resonance with the s-p state transition and 共B兲 to apply the method demonstrated in the experiment of Browaeys et al. 关9兴 by accelerating atoms in a lattice. We may also add a third possible approach—that is, 共C兲 to sweep atoms adiabatically across a Feshbach resonance. Köhl et al. 关10兴 ...
Presentation Slides
Presentation Slides

L - Jefferson Lab
L - Jefferson Lab

ppt
ppt

... Semi-unification, Weinberg-Salam model. The disparity between 10^{-2} and 10^{-6} is solved by symmetry breaking in gauge theory. 1960’s-1970’s (`t Hooft, Veltman, Nobel prize in 1999, total Five Nobel medals for this unification.) ...
or string theory
or string theory

Effective Field Theories, Reductionism and Scientific Explanation Stephan Hartmann
Effective Field Theories, Reductionism and Scientific Explanation Stephan Hartmann

Kaon Condensation
Kaon Condensation

N =1
N =1

... how SUSY breaking is fed (mediated) to the light particles determines their spectrum. This will be studied at the LHC. • Today, we’ll focus on supersymmetry breaking. ...
Metastable Supersymmetry Breaking
Metastable Supersymmetry Breaking

Phase transition in gauge theories, monopoles and the Multiple
Phase transition in gauge theories, monopoles and the Multiple

Holographic thermalization of quark gluon plazma
Holographic thermalization of quark gluon plazma

Weak Interactions - University of Tennessee Physics
Weak Interactions - University of Tennessee Physics

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Technicolor (physics)

Technicolor theories are models of physics beyond the standard model that address electroweak gauge symmetry breaking, the mechanism through which W and Z bosons acquire masses. Early technicolor theories were modelled on quantum chromodynamics (QCD), the ""color"" theory of the strong nuclear force, which inspired their name.Instead of introducing elementary Higgs bosons to explain observed phenomena, technicolor models hide electroweak symmetry and generate masses for the W and Z bosons through the dynamics of new gauge interactions. Although asymptotically free at very high energies, these interactions must become strong and confining (and hence unobservable) at lower energies that have been experimentally probed. This dynamical approach is natural and avoids issues of Quantum triviality and the hierarchy problem of the Standard Model.In order to produce quark and lepton masses, technicolor has to be ""extended"" by additional gauge interactions. Particularly when modelled on QCD, extended technicolor is challenged by experimental constraints on flavor-changing neutral current and precision electroweak measurements. It is not known what is the extended technicolor dynamics.Much technicolor research focuses on exploring strongly interacting gauge theories other than QCD, in order to evade some of these challenges. A particularly active framework is ""walking"" technicolor, which exhibits nearly conformal behavior caused by an infrared fixed point with strength just above that necessary for spontaneous chiral symmetry breaking. Whether walking can occur and lead to agreement with precision electroweak measurements is being studied through non-perturbative lattice simulations.Experiments at the Large Hadron Collider are expected to discover the mechanism responsible for electroweak symmetry breaking, and will be critical for determining whether the technicolor framework provides the correct description of nature. In 2012 these experiments declared the discovery of a Higgs-like boson with mass approximately 7002125000000000000♠125 GeV/c2; such a particle is not generically predicted by technicolor models, but can be accommodated by them.
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