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Pair production processes and flavor in gauge
Pair production processes and flavor in gauge

... the impact of sub-leading contributions. We find that only for very heavy fermions in the final state, especially top quarks, sizable corrections could emerge. This gives an interesting, possibly experimentally testable, scenario for the formal field theory underlying the electroweak sector of the s ...
Deflection of Beta Particles in Magnetic Field
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... this constant force perpendicular to the velocity vector. This force to change the direction of charged particles and follow a circular path at constant velocity in the magnetic field. So that the magnetic field cause Beta particles to change direction as the particles cross this field. ...
PROBset2_2014 - University of Toronto, Particle Physics and
PROBset2_2014 - University of Toronto, Particle Physics and

... of the Higgs in detail, as the colliding electrons and positrons will have well defined momenta. To go to even higher energies than the LHC, a Muon Collider has been proposed. This would be a synchrotron storage ring colliding   and   head on. a) How would you produce the muons necessary to inje ...
quarks and leptons - answers to practice questions
quarks and leptons - answers to practice questions

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E-Infinity theory and the Higgs field - SelectedWorks

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... mechanics also provides for a theory of the structure of atoms in terms of the electromagnetic forces between the atomic nucleus and the electrons orbiting them. In 1963 Sheldon Glashow proposed that the weak nuclear force and electricity and magnetism could arise from a partially unified electrowea ...
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physics phenomena accompanied streamlining of a body by the gas
physics phenomena accompanied streamlining of a body by the gas

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Standard Model



The Standard Model of particle physics is a theory concerning the electromagnetic, weak, and strong nuclear interactions, as well as classifying all the subatomic particles known. It was developed throughout the latter half of the 20th century, as a collaborative effort of scientists around the world. The current formulation was finalized in the mid-1970s upon experimental confirmation of the existence of quarks. Since then, discoveries of the top quark (1995), the tau neutrino (2000), and more recently the Higgs boson (2013), have given further credence to the Standard Model. Because of its success in explaining a wide variety of experimental results, the Standard Model is sometimes regarded as a ""theory of almost everything"".Although the Standard Model is believed to be theoretically self-consistent and has demonstrated huge and continued successes in providing experimental predictions, it does leave some phenomena unexplained and it falls short of being a complete theory of fundamental interactions. It does not incorporate the full theory of gravitation as described by general relativity, or account for the accelerating expansion of the universe (as possibly described by dark energy). The model does not contain any viable dark matter particle that possesses all of the required properties deduced from observational cosmology. It also does not incorporate neutrino oscillations (and their non-zero masses).The development of the Standard Model was driven by theoretical and experimental particle physicists alike. For theorists, the Standard Model is a paradigm of a quantum field theory, which exhibits a wide range of physics including spontaneous symmetry breaking, anomalies, non-perturbative behavior, etc. It is used as a basis for building more exotic models that incorporate hypothetical particles, extra dimensions, and elaborate symmetries (such as supersymmetry) in an attempt to explain experimental results at variance with the Standard Model, such as the existence of dark matter and neutrino oscillations.
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