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The Standard Model - Stony Brook University
The Standard Model - Stony Brook University

hewett
hewett

The New Minimal Standard Model
The New Minimal Standard Model

... constructed in this spirit, and it is a useful exercise to follow through with the same logic at the advent of the major discoveries we have witnessed. Of course, we require it to be a consistent Lorentz-invariant renormalizable four-dimensional quantum field theory, the way the MSM was constructed. ...
Direct Search of Dark Matter in High
Direct Search of Dark Matter in High

Lecture 5: Physics Beyond the Standard Model and Supersymmetry
Lecture 5: Physics Beyond the Standard Model and Supersymmetry

... • The W and Z masses depend very sensitively on the parameters that we use to characterize short distance physics → The model is not robust – As with any model, ultrasensitivity to input parameters is a sign that essential features are not properly understood Why New Physics at the LHC? • Need somet ...
English (MS Word) - CMS DocDB Server
English (MS Word) - CMS DocDB Server

... significance of five standard deviations (5 sigma)[3] above background expectations. The probability of the background alone fluctuating up by this amount or more is about one in three million. The evidence is strongest in the two final states with the best mass resolution: first the two-photon fina ...
1 - VideoLectures.NET
1 - VideoLectures.NET

Slides - Indico
Slides - Indico

... Without gravity one could have said that the problem is not so severe: After all, the theory must have a scale and it happens to be around 100GeV. But with gravity there is a very little flexibility. In Einstein’s gravity MP is the scale where gravitational interactions of elementary particles beco ...
New breakthroughs in physics expected at CERN
New breakthroughs in physics expected at CERN

The Weak and Strong Nuclear Interactions
The Weak and Strong Nuclear Interactions

Production Mechanism of Quark Gluon Plasma in Heavy Ion
Production Mechanism of Quark Gluon Plasma in Heavy Ion

... soft and semi-hard partons. It is unlikely that pQCD will be a valid approximation. ¾ Moreover even at equilibration we do not have an ideal gas or a small perturbation over that. ...
Physical Origin of Elementary Particle Masses
Physical Origin of Elementary Particle Masses

... 18 free parameters, and several more if neutrinos are non-massless, most of them related to the theoretically incalculable masses. In supersymmetric extensions of the standard model the free parameters rank in the number of hundreds, or more, again mainly connected to new (unobserved) masses of supe ...
The Phase Diagram of Nuclear Matter
The Phase Diagram of Nuclear Matter

Lecture notes 6: Strong and weak interactions
Lecture notes 6: Strong and weak interactions

PHY492: Nuclear & Particle Physics Lecture 18 Quark-onium QCD basics
PHY492: Nuclear & Particle Physics Lecture 18 Quark-onium QCD basics

Introduction to Effective Field Theory
Introduction to Effective Field Theory

... at high energy. (2) Start from the heaviest particle , integrate it out, calculating the matching condition. (3) Use RG to scale down to the next heaviest particle (4) We have a sequence of effective field theories. ...
The Universal Law of Gravitation
The Universal Law of Gravitation

Lecture 1, Introduction
Lecture 1, Introduction

quarks
quarks

... 1926 Schroedinger develops wave mechanics, which describes the behavior of quantum systems for bosons. Born gives a probability interpretation of quantum mechanics.G.N. Lewis proposes the name "photon" for a light quantum. 1927 Certain materials had been observed to emit electrons (beta decay). Sinc ...
Document
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Higgs-Boson-Arraigned
Higgs-Boson-Arraigned

Basic Ideas for Particle Properties
Basic Ideas for Particle Properties

Computation of hadronic two-point functions in Lattice QCD
Computation of hadronic two-point functions in Lattice QCD

Supersymmetry and Lorentz Invariance as Low-Energy
Supersymmetry and Lorentz Invariance as Low-Energy

... gravity fermionic fields spacetime. ...
SOME ASPECTS OF STRANGE MATTER : STARS AND
SOME ASPECTS OF STRANGE MATTER : STARS AND

< 1 ... 39 40 41 42 43 44 45 46 47 ... 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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