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Where can neutrino physics lead us?
Where can neutrino physics lead us?

... the presence of “matter effect background”) • Is it due to the Dirac phase in the MNS matrix? • Exactly the same question being addressed by Bfactories – i.e., K can be explained by the KM phase, but is it? – Cross check in a different system, e.g., B  Yes! – Is there new interaction (e.g. SUSY lo ...
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the standard model - Public < RHUL Physics Department TWiki
the standard model - Public < RHUL Physics Department TWiki

... • One of the consequences of this is that the gauge bosons acquire a mass and can thus be applied to weak interactions. • Spontaneous symmetry breaking and the Higgs mechanism has another extremely important consequence. It leads to a renormalisable theory with massive vector bosons. ⇒ Theory is re ...
Microscopic Realization of 2-Dimensional Bosonic Topological
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... The sign change of b02 under time reversal can be compensated by a gauge transformation b02 → −b02 . When averaging all the gauge fluctuations, the vortex condensate has a zero expectation value hb02 i = 0 [44]. In this way, we conclude that time reversal symmetry in not broken in the ground state e ...
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... interaction an electromagnetic one. One might separate electricity and magnetism only under special circumstances, they reveal themselves to us as the two sides of the same medal. At the same time phenomena become admissible, where electricity and magnetism occur simultaneously in a symmetric fashio ...
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Supersymmetry

Supersymmetry (SUSY), a theory of particle physics, is a proposed type of spacetime symmetry that relates two basic classes of elementary particles: bosons, which have an integer-valued spin, and fermions, which have a half-integer spin. Each particle from one group is associated with a particle from the other, known as its superpartner, the spin of which differs by a half-integer. In a theory with perfectly ""unbroken"" supersymmetry, each pair of superpartners would share the same mass and internal quantum numbers besides spin. For example, there would be a ""selectron"" (superpartner electron), a bosonic version of the electron with the same mass as the electron, that would be easy to find in a laboratory. Thus, since no superpartners have been observed, if supersymmetry exists it must be a spontaneously broken symmetry so that superpartners may differ in mass. Spontaneously-broken supersymmetry could solve many mysterious problems in particle physics including the hierarchy problem. The simplest realization of spontaneously-broken supersymmetry, the so-called Minimal Supersymmetric Standard Model, is one of the best studied candidates for physics beyond the Standard Model.There is only indirect evidence and motivation for the existence of supersymmetry. Direct confirmation would entail production of superpartners in collider experiments, such as the Large Hadron Collider (LHC). The first run of the LHC found no evidence for supersymmetry (all results were consistent with the Standard Model), and thus set limits on superpartner masses in supersymmetric theories. Whilst many remain enthusiastic about supersymmetry, this first run at the LHC led some physicists to explore other ideas. In any case, in 2015 the LHC resumed its search for supersymmetry and other new physics in its second run.
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