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GlueX Photon Beam Preparation
GlueX Photon Beam Preparation

Formal Expressions for the Electromagnetic Potentials in Any Gauge
Formal Expressions for the Electromagnetic Potentials in Any Gauge

Macroscopic Effects of the Quantum Trace Anomaly
Macroscopic Effects of the Quantum Trace Anomaly

Nanostructured Carbon Allotropes as Weyl
Nanostructured Carbon Allotropes as Weyl

String Backgrounds
String Backgrounds

Slides
Slides

... choice of the form of the E-M tensor, because to add a surface term will not change the conservation law satisfied by the E-M tensor. • The symmetric one is prefered because it is gauge invariant and the Einstain gravitation equation needs symmetric one. • In fact the E-M tensor density of em-field ...
Gapless layered three-dimensional fractional quantum Hall states
Gapless layered three-dimensional fractional quantum Hall states

... and the Coulomb interaction are both of paramount importance in such a putative phase. This poses a theoretical challenge since the obvious FQH states—such as those constructed from Chern-Simons mean-field theory—have a fixed number of electrons in each layer and are therefore unnatural except for v ...
parity-violating electron scattering
parity-violating electron scattering

Document
Document

briancox
briancox

... • Simulations (Louvain) indicate precision is better than necessary (theoretical limit is LHC beam energy uncertainty , s0 = 0.77 GeV ~ 50 microns) (also WW, M> 200 GeV, s100 fb -> very high sensitivity to anomalous quartic couplings) ...
The Matter Glitch
The Matter Glitch

... a. Why don’t protons decay as neutrons do? b. Why is the universe made of matter and not anti-matter? c. Why do neutrinos have a tiny but variable mass? a. Why are there three particle “generations” then no more? b. Why do electrons "half spin"? c. Why does mass vary enormously but charge doesn’t? d ...
The Matter Glitch
The Matter Glitch

Topological insulators and superconductors
Topological insulators and superconductors

Gauges - ETH Zürich
Gauges - ETH Zürich

Dark Z boson and Parity Violation
Dark Z boson and Parity Violation

The `Little Bang` in the Laboratory
The `Little Bang` in the Laboratory

Mean Multiplicity of Quark and Gluon Jets as a Function of Opening
Mean Multiplicity of Quark and Gluon Jets as a Function of Opening

... A comparison of the properties of quark and gluon jets has been made by Monte Carlo simulation of the reaction Z → bbg. The jet energy is held fixed for every 5 GeV between 15–30 GeV energies and the mean multiplicity of b-quark and gluon jets are obtained as function of the angle between them. It i ...
HIC: ALICE, The Wonderland more or less personal view
HIC: ALICE, The Wonderland more or less personal view

On the Topological Origin of Entanglement in Ising Spin Glasses
On the Topological Origin of Entanglement in Ising Spin Glasses

CERN Teacher Programmes: Welcome to CERN!
CERN Teacher Programmes: Welcome to CERN!

... exchange speculations: physicists looked at various combinations of charge exchange and spin exchange between nucleons with varying degrees of success, but none could produce complete and satisfactory quantitative explanations of observed nuclear phenomena. The way out of the difficulties was provid ...
neutrino
neutrino

New insights into soft gluons and gravitons. In
New insights into soft gluons and gravitons. In

cp violation and the origins of matter
cp violation and the origins of matter

20070822140014201
20070822140014201

... context of QCD. At the chiral phase transition we provide compelling evidence from lattice and phenomenological instanton liquid models that the QCD Dirac operator undergoes a metal - insulator transition similar to the one observed in a disordered conductor. This suggests that Anderson localization ...
Axion thermalization in the early universe
Axion thermalization in the early universe

... attached to the fermion line with the usual derivative coupling. The other reason is that color and flavor factors make the interaction rate larger. Our result in Eq. 共41兲 is in fact conservative. This is due to the fact that the effective theory below the scale F a has couplings of the axion to the ...
< 1 ... 6 7 8 9 10 11 12 13 14 ... 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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