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... Rubakov, Kuzmin, Shaposhnikov,... ...
Symmetry Breaking by Topology and Energy Gap
Symmetry Breaking by Topology and Energy Gap

Jet hadronization and E-by-E issues in energy loss
Jet hadronization and E-by-E issues in energy loss

Slides - indico.jinr.ru – Indico
Slides - indico.jinr.ru – Indico

A short review on Noether`s theorems, gauge
A short review on Noether`s theorems, gauge

pptx version - Physics Department, Princeton University
pptx version - Physics Department, Princeton University

... are just squares of the MNS matrix elements, independent of time/distance. However, most “observations” of state X do not determine its energy so precisely that the above scenario holds. Example: In a nuclear beta decay, A  A’ e e, the interaction of A’ and e with nearby atoms does not “measure” t ...
Large Extra Dimensions - Are you sure you want to look at this?
Large Extra Dimensions - Are you sure you want to look at this?

The Confinement Problem in Lattice Gauge Theory
The Confinement Problem in Lattice Gauge Theory

Top Physics
Top Physics

Elementary Particle Physics
Elementary Particle Physics

... (1) Mesons consist of qq and baryons of qqq. (2) Quarks carry a quantum number: isospin. The u, d  u , d  quarks represent different projections of the same quark (antiquark) in an internal isospin space, as p, n. When adding different isospins to form a hadron nature uses SU(2) symmetry to determ ...
Colloquium Slides
Colloquium Slides

PPT - Physics
PPT - Physics

Anisotropic pyrochlores and the global phase diagram of the checkerboard... Oleg A. Starykh, Akira Furusaki, and Leon Balents
Anisotropic pyrochlores and the global phase diagram of the checkerboard... Oleg A. Starykh, Akira Furusaki, and Leon Balents

The Standard Model of particle physics and beyond.
The Standard Model of particle physics and beyond.

... In addition, the associated antiparticles. The only difference between generations lies in the (increasing) mass. Experimental status [Particle Data Group Review]. * All these particules have been observed. * Last ones: top quark (1995) and tau neutrino (2001). The Standard Model of particle physics ...
CLASSICAL GAUGE FIELDS
CLASSICAL GAUGE FIELDS

Section D: - Curved Force Line Elements Theory
Section D: - Curved Force Line Elements Theory

The wavelet approach to peak finding
The wavelet approach to peak finding

... Now we can transform the invariant mass spectrum to G4 domain (a,b), find there bmax amax of the obtained surface and then fit it by the analytical formula for WG4(a,b;x0,σ)g starting fit from x0= bmax and σ = amax/3. To test this approach we prepared the simulated spectrum of invariant mass, consis ...
Exotic ccbar Resonances
Exotic ccbar Resonances

decoupling limit
decoupling limit

...  Within the solar system, p reaches the scale L … How can we trust the EFT at that scale ???  The breakdown of the EFT is not measured by the ...
Bridgeman, Alice - 2008
Bridgeman, Alice - 2008

Sinyatkin
Sinyatkin

SYMMETRIES IN PHYSICS: Philosophical Reflections
SYMMETRIES IN PHYSICS: Philosophical Reflections

... The formal context of Noether’s theorems is Lagrangian field theory wherein equations of motion are obtained through  a variational procedure (Hamilton’s principle) from the action integral, S = L d x. Noether’s theorems are discussed in detail in Earman (2002) and Brading and Brown (this volume). N ...
Notes for course on Physics of Particles and Fields, CMI, Autumn
Notes for course on Physics of Particles and Fields, CMI, Autumn

... of quarks and gluons. • Roughly, an elementary particle is one that may be treated as a point particle (or at least one with fixed shape) with fixed properties and with no sub-structure for the purposes under consideration. Any system (like an atom, nucleus or perhaps even a black hole) in its groun ...
here.
here.

Moti relativi
Moti relativi

< 1 2 3 4 5 6 7 8 9 10 ... 56 >

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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