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Flavour symmetry -- 50 years after SU(3)
Flavour symmetry -- 50 years after SU(3)

The Higgs Boson - Particle Physics Group
The Higgs Boson - Particle Physics Group

Syllabus PHYS 441
Syllabus PHYS 441

... 2. Limits on violation of Lorentz and CPT invariance in elementary interactions 3. A perfect liquid: the “quark-gluon plasma” observed in heavy ion collisions 4. Is the “Higgs” boson an elementary (point-like) object? 5. Utility of an inferred imbalance in transverse momentum in particle collisions. ...
Dark Matter and Dark Energy - Hitoshi Murayama Home Page
Dark Matter and Dark Energy - Hitoshi Murayama Home Page

K.K. Gan  Physics 780.02: Introduction to High Energy Physics
K.K. Gan Physics 780.02: Introduction to High Energy Physics

brown - Stony Brook University
brown - Stony Brook University

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HEP_Theory

... is to understand the ultimate building blocks of nature ...
Muon Lifetime
Muon Lifetime

... Fermi created a theory of beta decay [weak interactions] in 1933 after Pauli’s neutrino hypothesis was publicly presented. It was modified in the later 1950s to include parity violation and works quite well at low energies. It assumes that weak interactions happen at 4 fermion vertex with an interac ...
asu-higgs-temp1 - Experimental Elementary Particle Physics
asu-higgs-temp1 - Experimental Elementary Particle Physics

...  The Standard Model unifies the strong, weak, and electromagnetic interactions in the sense that they all arise from a local symmetry principle ...
What lies beyond? - University of Toronto Physics
What lies beyond? - University of Toronto Physics

Chapter 17 - Ferment Magazine
Chapter 17 - Ferment Magazine

... energy levels of 100 billion electron volts before they can be detected. Incredibly, like the Z+ , the particle predicted by the electroweak theory of Salam, Glashow and Weinberg that has been 1so-called ...
Higgs - mechanism
Higgs - mechanism

A first view on the mathematical structure of the standard
A first view on the mathematical structure of the standard

Classically conformal BL extended Standard Model
Classically conformal BL extended Standard Model

Asymptotic Freedom: From Paradox to Paradigm
Asymptotic Freedom: From Paradox to Paradigm

Prospects For LHC Physics
Prospects For LHC Physics

The Big Bang, the LHC and the Higgs boson
The Big Bang, the LHC and the Higgs boson

... We suspect the vacuum is full of another sort of matter that is responsible – the higgs…. a new sort of matter – a scalar? ...
20071008133014301
20071008133014301

... What if our theories are wrong and there is no higgs? Without the higgs our theory of WW interactions predicts scattering cross sections greater than one… there must be something there… What could it be? – extra space-time dimensions - a bigger gauge symmetry SU(2)xSU(2)x… - something new… ...
Standard Model of Physics
Standard Model of Physics

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The Standard Model (SM) describes the fundamental particles of the

... Leptons – These are particles with integer electric charge values and can be found alone. The six leptons are: the electron, muon, tau, electron neutrino, muon neutrino, and tau neutrino. Like quarks, each lepton has an associated anti-particle. ...
Dia 1
Dia 1

Physics Beyond the Standard Model
Physics Beyond the Standard Model

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Supercomputing in High Energy Physics
Supercomputing in High Energy Physics

... – without it, the WW scattering amplitude becomes infinite at energies of ~ 1 TeV • real experiments in the next decade would see this! ...
Slides - Antimatter
Slides - Antimatter

... Gauge theory Unified field theory of e and w forces Salaam, Weinberg, Glashow Single interaction above 100 GeV Mediated by W,Z bosons Predictions • Weak neutral currents (1973) • W and Z gauge bosons (CERN, 1983) ...
< 1 ... 51 52 53 54 55 >

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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