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Supersymmetry (SUSY) is an extension of the Standard Model which was introduced to cancel out some divergencies in quantum-mechanical calculations of the Higgs boson mass (mass hierarchy problem). SUSY relates fermions and bosons by transforming fundamental particles into "superpartners" which differ from the original particles by 1/2 unit of spin. The spin-0 partners of quarks and leptons are called squarks and sleptons (short for scalar quarks and scalar leptons). The spin-1/2 partners of gluons are called gluinos, and so on. If SUSY were an exact symmetry, a particle and its superpartner would have the same mass. This is obviously excluded experimentally, and thus SUSY must be a broken symmetry. No superpartners have been found so far. The lightest SUSY particles are believed to be in the mass range ~ 1 TeV or below. SUSY also provides a framework for attempts to unify electromagnetic, weak, strong, and gravitational interactions. It turns out that the superpartners modify the observed strengths of the electromagnetic, weak, and strong interactions in such a way that their inherent strengths become equal at very short distances (grand unification). It would be really neat if this was indeed the case!
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| MSSM | The "minimal" supersymmetric model (MSSM) assumes that all particles carry a conserved multiplicative quantum number, called R-parity, which is +1 for ordinary particles and -1 for superpartners. This would imply that SUSY particles are produced in pairs, and that there is a lightest supersymmetric particle (LSP) which is absolutely stable. The LSP's would have to be neutral and weakly interacting, i.e. much like heavy neutrinos. They would not interact in a detector, leading to apparent missing energy. The LSP's are natural candidates for dark matter, the stuff that supposedly holds galaxies together and accounts for most of the mass in the universe.
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| SUSY signal |
If SUSY particles exist, the decays of pair-produced sparticles would often result in final states with two or more jets and with two LSP's which would escape the detector. A "classic" SUSY signal would then be large missing energy in association with jets and/or isolated leptons. We will search for such a signal using PDE and dPDE. Numerous other signatures are also possible, of course, and we'll be on the lookout for any kind of new physics.
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