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hwk9
hwk9

... 1. A positively charged particle is moving horizontally when it enters the region between the plates of a capacitor, as the drawing illustrates. (a) Draw the trajectory that the particle follows in moving through the capacitor. (b) When the particle is within the capacitor, which of the following fo ...
Outline Solutions to Particle Physics Problem Sheet 1
Outline Solutions to Particle Physics Problem Sheet 1

... Le , Lµ , Lτ , total lepton number L = Le + Lµ + Lτ (and electric charge!) They are conserved in all interactions. 3. What quantum numbers are associated with quarks, and how are they defined? Are they conserved in strong, weak and electromagnetic interactions? • Total quark number, Nq = N (q) − N ( ...
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Historical Perspective
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... where are these corrections experimentally? Two solutions: - There are lots of new particles which cancel each other: supersymmetry. This is what huge crowds of theorists liked; in 2 y we will see if this is so! - There are no new particles: no correction, problem solved… until MP and QG Desert betw ...
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here:

... in a collaboration with Gell-Mann in 1961 . From the recently developing ideas of current algebra we showed that a gauge theory of weak interactions would inevitably run into the problem of strangeness-changing neutral currents. We concluded that something essential was missing. Indeed it was. Only ...
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High Energy Physics Summer School, Svit, Slovakia 3
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... constitute a family of elementary particles from which the known matter in the universe is built. The neutrino plays a role in the so-called weak decay of particles through the exchange of yet another set of force particles, which have large masses coming from the Higgs field. The recent likely disc ...
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... observations lead to some very interesting puzzles which will require some new ideas to address. It will, in fact, be our goal to solve these puzzles. The basic building blocks of the Universe are particles interacting via the exchange of bosons. We will throughly investigate the fundamental interac ...
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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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