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Particle physics, from Rutherford to the LHC
Particle physics, from Rutherford to the LHC

... denominators proportional to powers of some mass, because the Lagrangian density itself must have dimensionality equal to four. If the effective field theory arises from “integrating out” high-energy degrees of freedom in an underlying fundamental theory (or at least a more fundamental theory), then ...
Flavour from accidental symmetries
Flavour from accidental symmetries

Lecture 1
Lecture 1

... 1954 Yang and Mills develop a new class of theories called “gauge theories.” Although not realized at the time, this type of theory now forms the basis of the Standard Model. 1955 Chamberlain and Segre discover the antiproton. 1957 Schwinger writes a paper proposing unification of weak and electroma ...
Lecture notes 7: Strong and weak interactions
Lecture notes 7: Strong and weak interactions

Homework Set No. 4, Physics 880.02
Homework Set No. 4, Physics 880.02

LECTURE 22 THE STRONG COUPLING CONSTANT, QUARK-GLUON PLASMA (QGP)
LECTURE 22 THE STRONG COUPLING CONSTANT, QUARK-GLUON PLASMA (QGP)

Little Higgs dark matter and its collider signals
Little Higgs dark matter and its collider signals

PowerPoint ******
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... nonzero strength everywhere (including otherwise empty space), which in its vacuum state breaks the weak isospin symmetry of the electroweak interaction. When this happens, three components of the Higgs field are "absorbed" by the SU(2) and U(1) gauge bosons (the "Higgs mechanism") to become the lon ...
LHCtalkS08
LHCtalkS08

... – Quarks (>104:1) will become (~105:1)  There are some subtleties: if this is substructure, its nature is different than past examples. ...
SEARCHES FOR NEW PARTICLES AT THE LHC
SEARCHES FOR NEW PARTICLES AT THE LHC

Schwennesen Fundamental Particles and the Physics of the
Schwennesen Fundamental Particles and the Physics of the

... actually disturbances of the given force’s field caused by interactions between particles subject to the force [0, p. 208]. The most well-known of these force carriers is the photon, the mediator of the electromagnetic force, which has zero mass and travels at the speed of light [6, p. 114]. The exc ...
Higgs - Transcript - the Cassiopeia Project
Higgs - Transcript - the Cassiopeia Project

... In classical physics these fields were often thought of as continuous, smoothly changing entities. ...
The Standard Model and its Simple Extensions
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Forces Fundamental interactions in particle physics
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Lattice QCD in Mainland China: Status and Perspectives
Lattice QCD in Mainland China: Status and Perspectives

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14. Elementary Particles

... of particles and complex interactions with six quarks, six leptons, and four force-mediating particles. It’s based on three independent interactions, symmetries and coupling constants. ...
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LECTURE 14 HADRONS PHY492 Nuclear and Elementary Particle Physics
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Sizes in the Universe - Indico

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Standard Model is an Effective Theory

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Outstanding questions: physics beyond the Standard Model
Outstanding questions: physics beyond the Standard Model

... this mechanism implied the existence of an unseen particle, now called the Higgs boson, which has become in some sense the Holy Grail of particle physics, and certainly the first target of the LHC. As an analogy as to how the Englert–Brout–Higgs mechanism works, let us imagine an infinite, featureless ...
< 1 ... 41 42 43 44 45 46 47 48 49 ... 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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